Optimization of gas turbine combustion systems low load performance on simple cycle and heat recovery steam generator applications

Provided herein is a system and method for tuning the operation of a turbine and optimizing the mechanical life of a heat recovery steam generator. Provided therewith is a turbine controller, sensor means for sensing operational parameters, control means for adjusting operational control elements. The controller is adapted to tune the operation of the gas turbine in accordance preprogrammed steps in response to operational priorities selected by a user. The operational priorities preferably comprise optimal heat recovery steam generator life.

Skip to: Description  ·  Claims  ·  References Cited  · Patent History  ·  Patent History
Description
CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation-in-part of U.S. application Ser. No. 13/542,222, filed on Jul. 5, 2012, which is a continuation-in-part of U.S. application Ser. No. 12/463,060 filed on May 8, 2009. This application also claims the benefit of U.S. Application Ser. No. 61/601,876, filed on Feb. 22, 2012. The contents of U.S. application Ser. Nos. 12/463,060, 13/542,222 and 61/601,876 are hereby incorporated by reference in their entirety.

TECHNICAL FIELD

The present disclosure relates to an automated system to sense the operating condition of a combustion system and to make preset adjustments to achieve desired operation of the turbine thru out an optimized load range.

BACKGROUND

Lean premixed combustion systems have been deployed on land based gas turbine engines to reduce emissions, such as NOx and CO. These systems have been successful and, in some cases, produce emission levels that are at the lower limits of measurement capabilities, approximately 1 to 3 parts per million (ppm) of NOx and CO. Although these systems are a great benefit from a standpoint of emission production, the operational envelope of the systems is substantially reduced when compared to more conventional combustion systems. As a consequence, the control of fuel conditions, distribution and injection into the combustion zones has become a critical operating parameter and requires frequent adjustment, when ambient atmospheric conditions, such as temperature, humidity and pressure, change. The re-adjustment of the combustion fuel conditions, distribution and injection is termed tuning.

Controlled operation of a combustion system generally employs a manual setting of the operational control elements of a combustor to yield an average operational condition. These settings may be input through a controller, which as used herein shall refer to any device used to control the operation of a system. Examples include a Distributed Control System (DCS), a fuel turbine controller, a programmable logical controller (PLC), a stand-alone computer with communication to another controller and/or directly to a system.

These settings are satisfactory at the time of the setup, but conditions may change and cause unacceptable operation in a matter of hours or days. Tuning issues are any situation whereby any operational parameters of a system are in excess of acceptable limits. Examples include emissions excursion outside of allowable limits, combustor dynamics excursion outside of allowable limits, or any other tuning event requiring adjustment of a turbine's operational control elements. Other approaches use a formula to predict emissions based on gas turbine's operating settings and select a set point for fuel distribution and/or overall machine fuel/air ratio, without modifying other control elements, such as fuel gas temperature. Still other approaches employ a remote connection to the site by tuning experts, that will periodically readjust the tune, from the remote location. These approaches do not allow for continuous timely variation, do not comprehensively take advantage of actual dynamics and emission data or do not modify fuel distribution, fuel temperature and/or other turbine control elements.

Another variable that impacts the lean premixed combustion system is fuel composition. Sufficient variation in fuel composition will cause a change in the heat release of the lean premixed combustion system. Such change may lead to emissions excursions, unstable combustion processes, or even blow out of the combustion system.

In recent years, over-capacity of power generation, even that using F-class firing temperature gas turbines, has resulted in much of the installed gas turbine fleet running in a cyclic mode versus baseload operation. This means that many gas turbine operators are forced to shut their equipment down overnight, when power prices are so low that the losses incurred running overnight far outweigh the costs of starting the equipment every morning. This operation process has an impact on the maintenance of the equipment as each stop/start cycle causes a resulting load cycle on the equipment.

To combat this situation, gas turbine operators are investigating ways of running their equipment overnight while incurring the smallest economic loss possible. One viable solution is to lower the minimum load a gas turbine can achieve while still maintaining acceptable emissions levels. This method of operation is commonly referred to as “Turndown.”

“Turndown” has been used within the power generation industry for many years. As such, nothing directly related to this mode of operation is included as part of this patent. What is novel is the approach used by the ECOMAX™ tuning controller to tune the combustion system while in turndown, as well as the method incorporated within ECOMAX™ to mitigate detrimental effects on the combined-cycle heat recovery steam generator (HRSG) caused by low steam flows and high gas turbine exhaust temperatures. The system is also applicable to simple cycle operation; however, most simple cycle systems are applied to peak power generation and have a desirable shut-down process in the operating plan.

Often, as gas turbine loads are reduced, HRSG steam flows reduce while gas turbine exhaust temperatures rise. This combination, in conjunction with inadequate intra-stage attemperation flow capacity, often results in excessively high HRSG outlet steam temperatures (steam turbine inlet steam temperatures). In many cases these steam temperatures approach material limitations and can lead to pre-mature component failure. On the other extreme, steam conditioning/attemperation systems with adequate condensate flows can provide enough condensate to keep the superheat outlet temperature within specifications at the point of entrance into a steam turbine; however, localized over-attemperation can occur. This over-attemperation often leads to condensate impacting directly on steam piping downstream of the attemperator, causing excessive thermal fatigue in the piping sections immediately downstream of desuperheaters/attemperators.

To date efforts have focused on manually (if at all) modifying a gas turbine's fuel-to-air (f/a) ratio to keep the HRSG design constraints satisfied. However, factors such as ambient temperature changes, turbine component degradation, etc., can necessitate periodic manipulation of the gas turbine's f/a ratio, at low loads, to ensure acceptable HRSG inlet conditions. Automated manipulation of the f/a ratio of a gas turbine utilizing real-time HRSG operational information, as well as real-time gas turbine operational information, provides an efficient means to maximize HRSG component life.

It is understood that manipulation of a gas turbine's fuel-air ratio will directly affect the engine's “tune”, and as such any approach to accomplish this must be accompanied by another automated turbine control scheme to “re-tune” the turbine as-needed.

Mis-operation of the combustion system manifests itself in augmented pressure pulsations or increasing of combustion dynamics Pulsations can have sufficient force to destroy the combustion system and dramatically reduce the life of combustion hardware. Additionally, improper tuning of the combustion system can lead to emission excursions and violate emission permits. Therefore, a means to maintain the stability of the lean premixed combustion systems, on a regular or periodic basis, within the proper operating envelope, is of great value and interest to the industry. Additionally, a system that operates by utilizing near real-time data, taken from the turbine and HRSG sensors, would have significant value to coordinate modulation of fuel composition, fuel distribution, fuel gas inlet temperature, and/or overall machine f/a ratio (HRSG inlet temperature and airflow).

SUMMARY

Provided herein is a system and method for tuning the operation of a turbine and optimizing the mechanical life of a heat recovery steam generator. Provided therewith is a turbine controller, sensor means for sensing operational parameters, control means for adjusting operational control elements. The controller is adapted to tune the operation of the gas turbine in accordance preprogrammed steps in response to operational priorities selected by a user. The operational priorities preferably comprise optimal heat recovery steam generator life.

The present disclosure provides a controller and method for optimizing the fuel-air ratio of a gas-turbine combustor toward mitigating the detrimental effects of the turbine's exhaust conditions on the expected life of a Heat Recovery Steam Generator (HRSG) system, especially during low-load conditions. The gas turbine consumption system is of the type having sensor means for measuring operational parameters of the turbine and control means for controlling various operational elements of the turbine. The operational parameters of the turbine which are received by the controller include combustor dynamics, turbine exhaust temperature (overall fuel/air ratio), turbine exhaust emissions, and various heat recovery steam generator (HRSG) steam conditions. The operational control elements may include the fuel gas blend ratio (ratio of non-pipeline quality fuel gas to pipeline quality fuel gas), fuel distribution within the combustion system, fuel temperature and turbine exhaust temperature. The turbine/power plant system can also include a distributed control system (DCS) communicating with the sensor means and the control means. The tuning controller is normally connected to the turbine system through the DCS (although the tuning controller can connect directly to the gas turbine controller).

The tuning controller operates by receiving data from the sensor means. Operational priorities for the turbine are set within the controller and are typically selected from optimum NOx emissions, optimum power output, optimum combustor dynamics, optimum fuel gas blend ratio, and/or optimum HRSG life. The data received from the turbine sensors is compared to stored operational standards within the controller. The selected operational standards are based on the set operational priorities. A determination is made as to whether the turbine operation conforms to the operational standards. In addition, upon the data being out of conformance, a determination is made of the dominant tuning criteria again based on the preset operational priorities. Once the logical determinations are made, the tuning controller communicates with the operational control means through the DCS to perform a selected adjustment in an operational parameter of the turbine. The selected operational adjustment is based on the dominant tuning criteria and has a preset fixed incremental value and defined value range. Each incremental change is input over a set period of time, which is sufficient for the turbine to gain operational stability. Once the time period passes, operational data is again received from the turbine sensor means to determine if an additional incremental change is desired. Generally speaking, upon completing the adjustments within the defined range, a further operational parameter adjustment is selected, again based on the dominant tuning criteria, and a further fixed incremental adjustment is made within a defined range and over a set period of time. The tuning process continues by the controller receiving operational data to determine if the operation is conforming to the operational standards or whether an additional incremental adjustment is required. The operational parameters being adjusted by the tuning controller are preferably the fuel/air ratio within the gas turbine, the combustor fuel distribution split within the nozzles of the combustor, the fuel gas inlet temperature, and/or the fuel gas blend ratio.

It is understood that the tuning controller, when Optimum HRSG life is selected by the plant operator, will first evaluate what changes (if any) need to be made to the gas turbine f/a ratio to mitigate potential HRSG mechanical concerns and make these necessary changes. Subsequent to this optimization process, the tuning controller will tune the gas turbine, if needed, using the standard parameters of fuel splits, fuel gas temperature, and/or fuel gas composition (Note: gas turbine f/a ratio is not an option).

In a further aspect of the disclosure, the system performs a method for determination of the dominant gas turbine combustion system tuning scenario through the use of Boolean hierarchical logic and multiple levels of control settings.

In another aspect of the disclosure, the method performed relates to automated control of the gas turbine inlet fuel temperature through automated modification of the fuel gas temperature control set point within a Distributed Control System (DCS).

In a still further aspect of the disclosure, a method for automated control of a gas turbine inlet fuel temperature is defined by automated modification of the fuel gas temperature control set point within the fuel gas temperature controller.

In another aspect of the disclosure a method for communicating turbine control signals to a gas turbine controller is accomplished through the use of an existing gas turbine communication link with an external control device, such as, for example a MODBUS Serial or Ethernet communication protocol port existing on the turbine controller for communication with the Distributed Control System (DCS).

In a still further aspect of the disclosure a method for modification of a gas turbine combustion system is defined by a series of auto tuning settings via a user interface display, which utilizes Boolean-logic toggle switches to select user-desired optimization criteria. The method is preferably defined by optimization criteria based on Optimum Combustion Dynamics, Optimum NOx Emissions, Optimum Power, Optimum Heat Rate, Optimum CO Emissions, Optimum Heat Recovery Steam Generator (HRSG) Life, Optimum Gas Turbine Fuel Blend Ratio or Optimal Gas Turbine Turndown Capability whereby toggling of this switch changes the magnitude of the combustor dynamics control setting(s).

BRIEF DESCRIPTION OF DRAWINGS

For the purpose of illustrating the invention disclosed herein, the drawings show forms that are presently preferred. It should be understood that the invention is not limited to the precise arrangements and instrumentalities shown in the drawings of the present disclosure.

FIG. 1 shows an exemplary embodiment of a schematic representation of an operational plant communication system encompassing the gas turbine engine system, incorporating a gas turbine tuning controller as well as communication with various elements of the HRSG via plant DCS.

FIG. 2 shows an exemplary embodiment of a functional flow chart for the operation of a tuning controller according to the present disclosure.

FIG. 3 shows an exemplary embodiment of a user interface display for selecting the optimization mode within the present disclosure.

FIG. 4 shows an exemplary schematic of the inter-relationship of various optimization mode settings.

FIG. 5 shows an exemplary overview schematic of the process steps utilized to determine the alarm signals triggered according to the present disclosure.

FIG. 6 shows an exemplary process overview of the steps to determine allowable turbine tuning parameters.

FIG. 7 shows a further detailed exemplary process according to the steps shown in FIG. 6.

FIG. 8 provides a further detailed exemplary schematic of the steps the present disclosure utilizes to determine the dominant tuning concern.

FIG. 9 shows a first example schematic of the determination of the system's dominant tuning concern, given various alarm inputs into the present disclosure.

FIG. 10 shows a second example schematic of the determination of the system's dominant tuning concern, given various alarm inputs into the present disclosure.

FIG. 11 shows a third example schematic of the determination of the system's dominant tuning concern, given various alarm inputs into the present disclosure.

FIG. 12 shows a fourth example schematic of the determination of the system's dominant tuning concern, given various alarm inputs into the present disclosure.

FIG. 13 shows a first operational example of operational tuning of a gas turbine engine system as contemplated by the present disclosure.

FIG. 14 shows a second operational example of operational tuning of a gas turbine engine system as contemplated by the present disclosure.

FIG. 15 shows a third operational example of operational tuning of a gas turbine engine system as contemplated by the present disclosure.

FIG. 16 shows a fourth operational example of operational tuning of a gas turbine engine system as contemplated by the present disclosure.

DETAILED DESCRIPTION

The present disclosure generally relates to systems and methods for tuning the operation of combustion turbines. In the depicted embodiments, the systems and methods relate to automatic tuning of combustion turbines, such as those used for power generation. Persons of ordinary skill in the art will appreciate that the teachings herein can be readily adapted to other types of combustion turbines. Accordingly, the terms used herein are not intended to be limiting of the embodiments of the present disclosure. Instead, it will be understood that the embodiments of the present disclosure relate generally to the field of combustion turbines, and in particular for systems, methods and computer readable media for tuning of combustion turbines.

FIG. 1 is a communication diagram for a gas turbine engine (not shown), within which a tuning controller 10 of the present disclosure operates. A distributed control system (DCS) 20 serves as the main communication hub. As an alternative, a plant using the gas turbine controller as a DCS, may also have the tuning controller 10 communicate directly to the gas turbine controller 30. As a further alternative, the tuning controller 10 can communicate directly with the gas turbine controller 30, irrespective if the gas turbine controller 30 is functioning as a DCS. Most of the turbine control is performed through the DCS 20. A turbine controller 30 communicates directly with the gas turbine and with the DCS 20. In the present disclosure, information relevant to turbine operation, e.g., turbine dynamics, turbine exhaust emissions, etc. are directed through the DCS 20 to the tuning controller 10. The tuning controller 10 is contemplated to be a stand-alone PC used to run as a programmable logical controller (PLC). The tuning controller 10 is preferably a separate computer from the turbine controller 30 and does not normally communicate directly with the turbine controller 30, except through the DCS 20. However; as mentioned above, the tuning controller 10 can be configured to directly communicate with the gas turbine controller 30.

Referring now to FIGS. 1 and 2, the tuning controller 10 is contemplated to be a stand-alone PC used to run as a programmable logical controller (PLC). The tuning controller 10 is preferably a separate computer from the turbine controller 30 that is in constant communication from with the turbine controller 30. The signals from the tuning controller 10 may also be transferred to the turbine controller 30 or other controls within the system by the use of an external control device, such as a MODBUS Serial or Ethernet communication protocol port existing on or added to the system.

The relevant operational data is received from sensor means associated with the turbine. For example, the turbine exhaust emission reading is taken from stack emissions by a continuous emissions monitoring system (CEMS) 40, which is connected to the DCS. Combustion dynamics is sensed using a dynamic pressure sensing probe located within the combustion region of the turbine combustor. As shown, a continuous dynamics monitoring system (CDMS) 50 is provided and communicates with the DCS. The CDMS 50 preferably uses either direct mounted or wave guide connected pressure or light sensing probes to measure the combustion dynamics. Another relevant operational parameter is the fuel gas temperature. Again, this temperature information is directed to the tuning controller 10 through the DCS 20 from the fuel heating controller 60. Since part of the tuning operation may include adjustment of the fuel temperature, there may be a two-way communication between the tuning controller 10 and the fuel heating unit 60. The DCS 20 communicates with a fuel blend ratio controller 70 to adjust the ratio of pipeline quality gas to non-pipeline quality gas (for subsequent consumption within the gas turbine). There exists in direct communication between the fuel blend ratio controller 70 and the tuning controller 10 via the DCS 20. Last, as part of this disclosure, certain key operating parameters of the HRSG 80 are sent to the tuning controller 30 via the DCS 20. If the tuning controller 10 determines that various parameters of the HRSG 80 are outside of allowable ranges, changes to the gas turbine f/a ratio are sent from the tuning controller 10 through the DCS 20 to the gas turbine controller 30.

Relevant operational data from the turbine and HRSG is collected several times per minute. This data collection allows for near real-time system tuning. Most relevant turbine and HRSG operational data is collected by the tuning controller 10 in near real-time. However, the turbine exhaust emissions sensor means is typically received by the tuning controller 10 with a 2 to 8 minute time lag from current operating conditions. This time lag necessitates the need for the tuning controller 10 to receive and buffer relevant information, for a similar time lag, before making operational tuning adjustments. This tuning controller 10 tuning adjustment time lag assures that all of the operational (including exhaust emissions) data is representative of a stable turbine operation before and after any adjustments have been made. Once the data is deemed stable, the tuning controller 10 determines whether there is a need for adjustment of tuning parameters. If no adjustment is necessary, the tuning controller 10 maintains the current tuning and waits to receive the next data set. If changes are desired, tuning commences. First, HRSG operational data are compared against HRSG component mechanical limits. If any HRSG mechanical limits (or margin against such limits) are violated, the tuning controller 10 will alter the gas turbine f/a ratio through the DCS 20 to the turbine controller 30. Subsequently, if there is sufficient margin in the key operational characteristics of the gas turbine (namely exhaust emissions and combustor dynamics), the tuning controller 10 can send a command (if applicable) to the fuel gas ratio controller 70 (through the DCS 20) to increase the ratio of non-pipeline quality gas to pipeline quality gas.

All determinations of the need for turbine tuning are performed within the tuning controller 10. The tuning operation is started based on an “alarm” created by receipt of operational data outside of preset operational criteria. In order for the tuning operation to be initiated, the alarm—and thus the data anomaly—must continue for a predetermined period of time.

One example of a tuning adjustment is the variation of the fuel nozzle pressure ratio to adjust combustion dynamics. With the requirement of higher firing temperatures to achieve greater flame temperatures and efficiency, turbine combustors must release more energy in a given combustor volume. Better exhaust emissions are often achieved by increasing the mixing rate of fuel and air upstream of the combustion reaction zone. The increased mixing rate is often achieved by increasing the pressure drop at the fuel nozzle discharge. As the mixing rate increases in combustors, the turbulence generated by combustion often leads to noise within the combustor and may lead to the generation of acoustic waves. Typically, acoustic waves are caused when the sound waves of the combustion flames are coupled with the acoustic characteristics of the combustor volume or the fuel system itself.

Acoustic waves may affect the internal pressure in the chamber. Where pressure near a fuel nozzle rises, the rate of fuel flowing through the nozzle and the accompanying pressure drop decreases. Alternatively, a decrease in pressure near the nozzle will cause an increase in fuel flow. In cases where a low fuel nozzle pressure drop allows fuel flow oscillation, a combustor may experience amplified pressure oscillations. To combat the pressure oscillations within the combustor, combustion dynamics are monitored and the fuel air ratio and fuel nozzle pressure ratio may be modified to reduce or eliminate unwanted variations in combustor pressure, thereby curing an alarm situation or bringing the combustion system back to an acceptable level of combustion dynamics.

As shown in FIG. 2, the data received from the sensing means for the HRSG operational parameters (80), combustor dynamics (50), turbine exhaust emissions (40), and other relevant turbine operating parameters (30) are directed through the DCS (20) to the tuning controller (10). These input values are then compared to standard or target operational data for the turbine. The stored operational standards are based, at least in part, on the operational priority settings for the turbine. These priority settings are defined on the main user interface 12 of the tuning controller 10 and are shown graphically in FIG. 3. Based on the priority settings, a series of adjustments are made to the operation of the turbine by the turbine controller 10 connected through the DCS 20. The adjustments are directed to the control means, including the fuel heating unit 60 (FIG. 1), fuel blend ratio controller 70, and various other operational elements 90 of the turbine (FIG. 2).

The interface display 12 shown in FIG. 3 is comprised of switches (each having an On/Off indication). These switches allow the user to specify the desired tuning priorities for the operation of the turbine. The switched operational priorities include optimum NOx emissions 14, optimum power 16, optimum combustor dynamics 17, optimum fuel blend ratio 18, and optimum HRSG life 19. Each of these switches is set by the user to adjust the preferred operation of the turbine. Within the tuning controller are functions that operate within the priorities set by the switches. Preferably, if both the optimum NOx emissions switch 12 and the optimum power switch 14 are set to “On”, the controller 10 will run in the optimum NOx mode, not optimum power. Thus, to run in optimum power mode, the optimum NOx emissions switch 12 must be “Off”. Optimum dynamics 17 can be selected at any time. It is explicitly noted that other User-Interface Toggle Switches (not shown) may be used, including parameters such as Optimum Heat Rate, Optimum CO emissions, Optimum Heat Recovery Steam Generator (HRSG) Life, Optimum Gas Turbine Fuel Blend Ratio, Optimal Gas Turbine Turndown Capability, etc.

FIG. 4 shows a graphical representation of the interrelationship of the interface display switches. As shown, switching one parameter “On” will alter the alarm limits to a different level than their “Off” level. In the example shown in FIG. 4, the alarm limits are shown with both Optimum NOx and optimum power in the “On” position and in the “Off” position. These points on the graph are then modified by the selection of optimum dynamics (represented throughout by the symbol δ) in either the “On” or “Off” position. The points shown on the graph of FIG. 4 represent an exemplary set of limits for dynamics, based on the user's selected operational priorities.

Returning to FIG. 2, there is shown a representation of the logical flow of the determinations and calculations made within the tuning controller 10. The tuning controller 10 receives the actual operating parameters of the turbine through the turbine controller 30, combustor dynamics through the CDMS 50, turbine exhaust emissions through the CEMS 40, and relevant HRSG operating parameters 80. This sensor data is directed to the tuning controller 10 through the DCS 20. The received sensor data is compared to stored operational standards to determine if the turbine operation is conforming to the desired settings. The operational standards are based on the preset operational priorities of the turbine, defined by the switches 14, 16, 17, 18, and 19 on the main user interface display 12 of the tuning controller 10 (FIG. 3).

Based on the preset operational priorities, a hard-coded hierarchical Boolean-logic approach determines the dominant tuning criteria based on operational priorities. From this logical selection, the tuning controller 10 implements a fixed incremental adjustment value for changing an operational parameter of the turbine within a maximum range of adjustment (e.g., high and low values). The tuning changes are made in a consistent, pre-determined direction over a pre-determined increment of time and are dependent on the dominant tuning criteria at present. It is contemplated that no formulaic or functional calculations are made to determine the magnitude of tuning adjustments; rather, the incremental adjustments, the direction of the adjustments, the time span between adjustments, and the maximum range for the adjustments for each parameter and for each tuning criteria are stored in the tuning controller 10.

As shown in FIG. 2, when Optimum HRSG Life 19 is not selected by the operator, the tuning controller 10 determines whether the emissions are in compliance 100 and whether the combustor dynamics are at acceptable levels 102. If both are in compliance with the set operational standards, the tuning controller 10 waits for the next data set from the CEMS 40 or the CDMS 50, and for other turbine operational data 90. If both are in compliance with the set operational standards and possess sufficient operational margin, and Optimum Fuel Blend Ratio 18 is selected, the tuning controller 10 will send a command to the fuel blend ratio controller 70 to increase the ratio of non-pipeline quality gas to pipeline quality gas. If the received data is non-conforming with the operational standards, i.e. above or below alarm levels, as is the case with step 104 of FIG. 2, the tuning operation moves to the next tuning step of first determining the dominant tuning concern 106. The logical adjustment of turbine operation is defined by the dominant tuning criteria 106, which is based, at least in part, on the preset operational priorities set within the user interface 12, as will be discussed below with respect to FIG. 8.

If Optimum HRSG Life 19 is selected by the operator, the first decision the tuning controller makes is an assessment of the margin of pertinent HRSG parameters (including but not limited to high pressure superheat outlet steam temperature, hot reheat outlet steam temperature, high pressure superheat steam desuperheater margin against saturation (degrees Fahrenheit of temperature immediately downstream of attemperator compared to saturation temperature), hot reheat steam desuperheater margin against saturation) against design limits. These temperature margins are compared against allowable margins as defined by the user. If the actual temperature margins are less than the allowable margins, the tuning controller 10 will automatically adjust the turbine controller's f/a ratio 122. In this particular case, the tuning controller 10 has first adjusted the gas turbine's f/a ratio for an external reason (HRSG component life). This change can adversely affect the gas turbine's current state-of-tune. Therefore, the normal gas turbine tuning scheme is performed by the tuning controller 10; however, changes to the turbine's f/a ratio are not allowed. The remaining gas turbine tuning scheme is defined below.

In a preferred operation, the tuning controller 10 will first attempt to change the turbine combustor fuel splits 108. The fuel split determines the distribution of the fuel flow to the fuel nozzles in each combustor. It should be noted that while the current embodiment indicates the presence of two adjustable fuel circuits, this approach can be utilized for one, two or more fuel circuits. If these adjustments do not resolve the tuning issue and do not place the operational data back into conformance with the operational standards, a further adjustment is performed. In certain situations or if the efficacy of fuel split changes on resolving high combustor dynamics is low, the next incremental adjustment is a change of the fuel gas temperature set point. In this adjustment step, the tuning controller 10 sends a modified fuel gas inlet temperature signal to the DCS 20, which is directed to the fuel heating unit 60.

Referring again to FIG. 2, if modification of the combustor fuel splits and/or fuel gas inlet temperature does not resolve the tuning issue 110, the tuning controller 10 will then alter the overall fuel/air ratio 112. This approach makes changes to the turbine thermal cycle utilizing fixed incremental changes over pre-determined amounts of time. The step is intended to adjust the exhaust temperature (up or down) by adjusting the air to fuel ratio in accordance with predetermined, standard control curves for the turbine operation, which are maintained within the memory of the tuning controller 10. If changes made to the gas turbine's overall fuel/air ratio do not resolve the tuning issue 114 or if Optimum HRSG Life 19 is enabled and HRSG mechanical concerns exist, the tuning controller 10 will adjust the fuel blend ratio 116.

In the present disclosure, it is contemplated that all control changes directed by the tuning controller 10 are fed back to the turbine system (30, 90), fuel gas temperature controller 60, and fuel blend ratio controller 70 through the DCS 20. However, the tuning controller 10 can be configured to communicate directly with the turbine controller 30. These changes are implemented directly within the various controller means within the system or through the turbine controller 30. When the operational data is returned to the desired operational standards, the tuning settings are held in place by the tuning controller pending an alarm resulting from non-conforming data received from the sensor means through the DCS.

The adjustments sent from the tuning controller 10 to the turbine controller 30 or the associated controller (60, 70) means are preferably fixed in magnitude. Thus, the adjustments are not recalculated with new data or optimized to a target. The adjustments are part of an “open loop”. Once started, the adjustments move incrementally to the preset maximum or maximum within a specified range, unless an interim adjustment places the operation data into conformance with the operational standards. Under most circumstances, when the full incremental range for one operational parameter is completed, the tuning controller moves on to the next operational parameter, which is defined by the preset operational priorities. The specific order of operational control elements is not fixed, and can be determined by operational priorities. The logic of the tuning controller drives the operational control element adjustment based on a “look-up” table stored within the memory of the tuning controller and preset operational priorities.

The tuning controller preferably addresses one operational parameter at a time. For example, the dominant tuning criteria dictates the first adjustment to be made. In the preferred example discussed above, the fuel distribution/split parameter is first adjusted. As indicated in FIG. 2, the fuel split of fuel circuit 1 is first addressed, followed by the split for fuel circuit 2. Again, this method can be applied to any combustion system with one or more adjustable fuel circuits. The fuel gas inlet temperature adjustment generally follows the fuel split adjustments when needed. Within each step, there is an incremental adjustment, followed by a time lag to permit the adjusted turbine operation to stabilize. After the time lag, if the current operational data analyzed by the tuning controller indicates that turbine operation still remains outside of the operational standards, the next incremental adjustment within the step is made. This pattern repeats for each step. Under most circumstances, only when one adjustment step is completed does the tuning controller move onto the next operational parameter. It should be noted that there exists an over-riding loop whereby the tuning controller 10 will directly increase the non-pipeline quality gas blend ratio (through the fuel blend ratio controller 70) if key turbine operational characteristics possess ample operational margin (against alarm conditions) 118. The control methodology of this over-riding control loop is identical to that mentioned above for fuel splits and turbine f/a ratio—a change is made in a pre-defined direction, a pre-defined amount, in a pre-defined amount of time.

The tuning controller preferably controls combustion operation to maintain proper tuning in variable conditions of ambient temperature, humidity and pressure, all of which vary over time and have a significant effect on turbine operation. The tuning controller may also maintain the tuning of the turbine during variation in fuel composition. Variation in fuel composition may cause a change in the heat release, which can lead to unacceptable emissions, unstable combustion, or even blow out. The tuning controller will adjust the fuel composition entering the turbine indirectly through changes in the fuel blend ratio 116.

Another aspect regarding fuel splits within the combustor deals directly with combustion systems having a series of outer nozzles (of the same type, controlled by an outer fuel split affecting circumferential distribution of fuel within the outer fuel nozzles) in combination with a center nozzle (of same or different type compared to outer nozzles, controlled by an inner/center fuel split). Within this framework, the center nozzle can either operate with a “rich” or “lean” fuel-to-air ratio, as compared to the f/a of the outer fuel nozzles. Most combustion tuning keeps the combustion system either on a “lean center nozzle” or a “rich center nozzle” mode of operation. In some circumstances, better flame stability can be achieved with a “rich center nozzle” fuel split profile when compared to a “lean center nozzle”; however, this normally results in higher NOx emissions, Therefore, a hybrid fuel schedule is of particular interest, whereby the combustion system utilizes a “lean center nozzle” fuel split schedule at higher load conditions (where flame stability is less of a concern but NOx emissions are more of a concern) transitioning to a “rich center nozzle” fuel split schedule at lower load and turndown conditions (where flame stability is more of a concern and NOx is less of a concern). The system of the present disclosure determines which fuel split schedule is employed (rich or lean center nozzle) at each operating point (allowing for the use of a hybrid fuel split schedule), and adjusts the fuel split schedule (Fuel Circuit 1 Split and Fuel Circuit 2 Split) in the proper direction. Again, changes made are of fixed magnitude in fixed time intervals.

Another point regarding fuel splits deals directly with combustion systems having a series of outer nozzles (of same or different type, controlled by an outer fuel split affecting circumferential distribution of fuel within the outer fuel nozzles) with no center nozzle. Within this framework, a subset of these outer nozzles (referred to generally as minor circuit 1) can either operate with a “rich” or “lean” fuel-to-air ratio, as compared to the f/a of the remaining outer fuel nozzles (referred to as major circuit 1). Most combustion tuning keeps the combustion system either on a “lean minor circuit 1” or a “rich minor circuit 1” circumferential fuel split mode of operation. In some circumstances, better flame stability can be achieved with a “lean minor circuit 1” fuel split profile when compared to a “rich minor circuit 1” fuel split profile; however, this can result in higher NOx emissions. Therefore, a hybrid fuel schedule is of particular interest, whereby the combustion system may utilize a “rich minor circuit 1” fuel split schedule at higher load conditions (where flame stability is less of a concern but NOx emissions are more of a concern) transitioning to a “lean minor circuit 1” fuel split schedule at lower load and turndown conditions (where flame stability/CO is more of a concern and NOx is less of a concern). The system of the present disclosure determines which fuel split schedule is employed (rich or lean minor circuit 1) at each operating point (allowing for the use of a hybrid fuel split schedule), and adjusts the fuel split schedule (Fuel Circuit 1 Split and Fuel Circuit 2 Split, if applicable) in the proper direction. Again, changes made are of fixed magnitude in fixed time intervals.

One further aspect regarding fuel splits deals directly with combustion systems having one or more annular rings of fuel nozzles (of same or different type, controlled by an circumferential fuel split affecting circumferential distribution of fuel within each ring of fuel nozzles), whereby a second family of fuel splits may be available (if more than one annular ring of fuel nozzles exists) which adjusts the relative (radial) amount of fuel to each of the radially concentric fuel rings (ring 1, ring 2, etc.). Within this framework, a subset of each ring's fuel nozzles (referred to as minor circuit ring 1, minor circuit ring 2, etc.) can either operate with a “rich” or “lean” fuel-to-air ratio, as compared to the f/a of the remaining ring's fuel nozzles (referred to as major circuit ring 1, major circuit ring 2, etc.). Most combustion tuning keeps the combustion system either on a “lean minor circuit ring 1” or a “rich minor circuit ring 1” (and similar approaches for rings 2, 3, etc.) circumferential fuel split mode of operation. In some circumstances, better flame stability can be achieved with, using ring 1 as an example, a “lean minor circuit ring 1” fuel split profile when compared to a “rich minor circuit ring 1” fuel split profile; however, this can result in higher NOx emissions. Therefore, a hybrid fuel schedule is of particular interest, whereby the combustion system may utilize a “rich minor circuit ring 1” fuel split schedule at higher load conditions (where flame stability is less of a concern but NOx emissions are more of a concern) transitioning to a “lean minor circuit ring 1” fuel split schedule at lower load and turndown conditions (where flame stability/CO is more of a concern and NOx is less of a concern). The system of the present disclosure determines which fuel split schedule is employed for each ring, if applicable (rich or lean minor circuit ring 1, rich or lean minor circuit ring 2, etc.) at each operating point (allowing for the use of a hybrid fuel split schedule), and adjusts the fuel split schedule (Fuel Circuit 1 Split and Fuel Circuit 2 Split, if applicable) in the proper direction. Again, changes made are of fixed magnitude in fixed time intervals.

FIG. 5 provides a schematic that details the framework for determining the dominant tuning concern 106, as included in FIG. 2. Future steps will be described below with respect to FIG. 8. First, relevant emissions parameters 120 and combustor dynamics 122 are received by the tuning controller 10 from the CEMS 40 and CDMS 50, as detailed above. The relevant emissions parameters 120 and combustor dynamics 122 are then compared to allowable tuning limits 124 that are also provided to the tuning controller 10. The allowable tuning limits are in the form of preset ranges that may be adjusted using the tuning interface 12 of FIG. 3 and determined according to the logic set forth below with respect to FIGS. 6 and 7. The output of this comparison is a series of “True” alarms 126 of various tuning concerns, where an alarm condition is indicated if the sensed operational data 120, 122 is above or below a given alarm range set forth in the tuning limits 124.

Alarm conditions may have more than one level or tier. For example, there may be varying degrees of severity of an alarm, such as: high “H”; high-high “HH”; high-high-high “HHH” and low “L”; low-low “L”; low-low-low “LLL”. The “True” logical alarms 126 are subsequently ranked according to their level of importance (e.g. high-high “HH” alarms are more important than high “H” alarms, etc.) in step 130. If more than one tuning concern shares the same level, the tuning concerns will then be ranked according to the user preferences as set forth below with respect to FIG. 8. If only one “True” alarm emerges, this will be selected and used as the dominant tuning concern 106 to initiate the tuning process as set forth in FIG. 2. However, the results of the process of FIG. 5, namely the ranked “True” alarms 130, will be processed through user determined criteria, as shown in FIG. 8, before a dominant tuning concern 106 is confirmed.

In FIG. 6, a flow chart is provided to explain how the allowable tuning limits 124 are determined. Once determined, the tuning limits 124 are compared to the operational data 120, 122 as set forth above and shown in FIG. 5. First, the User Interface Toggle Switches 14, 16, 17 corresponding to those in the interface display 12 of FIG. 3, are compared against each other, utilizing an internal hierarchy to allow passage of the alarm constraints relative to the most significant toggle switch. Thus, depending on which switches are in the “On” position, different tuning limits will be included in the allowable tuning limits 124. Each of Optimum NOx, Optimum Power and Optimum Dynamics has a collection of preset limits (denoted by the numerals 134, 136 and 138 in FIG. 6), depending on whether the corresponding toggle switch 14, 16, 17 is in the “On” of “Off” position. There is also an internal set of default limits 140 to be used when none of the toggle switches are in the “On” position.

The internal hierarchy will determine which tuning limits shall take precedence in the event that competing toggle switches 14, 16 or 17 are in the “On” position. In the present example, the hierarchy ranks Optimum NOx 14 above Optimum Power 16. Optimum Dynamics 17 may be selected at any time and will simply alter the tuning limits of the other selections given, such as is shown in FIG. 4. If Optimum NOx 14 and Optimum Power 16 are both in the “On” position, the tuning limits for Optimum NOx 134 will be used. Additionally, the tuning limits for Optimum Dynamics 138 are utilized if this toggle switch 17 is activated. If no User Interface Toggle Switches 14, 16, 17 are active, default tuning limits 140 are provided as the allowable tuning limits 124. All of the tuning limits 134, 136, 138 and 140 that may be used to construct the allowable tuning limits for the tuning controller 10 may be developed by the end user and programmers and are then preferably hard coded into the tuning controller 10 for a given application. The methodology outlined in FIG. 6 is meant to provide an exemplary framework for incorporation of a number of different User Interface Toggle Switches, such as those options set forth above with respect to FIG. 3 including Optimum HRSG Life 19, whereby only a subset are specifically outlined in this disclosure.

FIG. 7 shows a specific example of the flow chart of FIG. 6 given for the determination of a subset of the system's allowable tuning limits. In this example, the tuning limits for High NOx, High HighNOx, High Class 1 δP's, High Class 2 δP's will be determined based on preset tuning limits and the user's preferences. The various exemplary tuning limits are provided for Optimum NOx 134, Optimum Power 136, Optimum Dynamics 138, and No Optimal Settings 140 are given corresponding numerical values (shown respectively in blocks 152, 154, 156 and 158). The corresponding numerical values given for each criterion vary, such that the allowable limits 124 will be different depending on which toggle switches 14, 16 or 17 are selected. By way of example, the Optimum NOx 134, 152 and Optimum Power 136, 154 give limits for NOx, but also provide limits for Dynamics that are to be used in the event that Optimum Dynamics 138, 156 is not selected. However, in the event that the Optimum Dynamics toggle 17 is selected, the Class 1 δP's and Class 2 δP's values provided therefore 156 shall be used instead of the values listed with respect to Optimum NOx 134, 152 and Optimum Power 136, 154.

In this particular example, the toggle switches for Optimum NOx 14 and Optimum Dynamics 17 are selected, with the switch for Optimum Power 16 left in the “Off” position. Thus, the values from Optimum NOx for High NOx and High HighNOx 152 are provided. Also, because Optimum Dynamics 17 is also selected, the Dynamics values for High Class 1 δP's and High Class 2 δP's 138, 156 replace those δP's values provided with respect to Optimum NOx 134, 152. As a result, the allowable tuning limits 124 are provided as shown in block 160. These allowable tuning limits 124 correspond to those used in FIG. 5, as described above, to determine whether information from the CEMS 40 and CDMS 50 is in an alarm state or operating normally.

FIG. 8, shows a further schematic for the process of incorporating a user's priorities and the “True” alarm conditions received for determining the dominant tuning concern 106. It is this tuning concern 106 which dictates the turbine operational changes the turbine controller 10 performs, as shown in FIG. 2.

First, a determination is made of all potential dominant tuning issues 142. These include, but are not limited to: combustor blowout, CO emissions, NOx emissions, Class 1 combustor dynamics (Class 1 δP's), Class 2 combustor dynamics (Class 2 δP's), and HRSG mechanical life, The list of potential dominant tuning issues 142 is determined by the user and programmer and may be based on a number of factors or operational criteria. By way of example, Class 1 and Class 2 combustor dynamics δP's refer to combustion dynamics occurring over specific ranges of acoustic frequencies, whereby the range of frequencies is different between Classes 1 and 2. Indeed, many combustion systems can possess different acoustic resonant frequencies corresponding to Class 1 and Class 2, and variations in these 2 dynamics classes may be mitigated utilizing different turbine operational parameter changes for each different turbine and/or combustor arrangement. It should also be noted that certain combustion systems may have none, 1, 2, or greater than 2 different “classes” (frequency ranges) of combustor dynamics which can be tuned. This disclosure utilizes a system whereby 2 different combustor dynamics classes are mentioned. However, it is fully intended that this disclosure can be broadly applied to any number of distinct dynamics frequency classes (from 0 to greater than 2).

After determination of the potential dominant tuning issues 142, these issues are ranked in order of significance 144 according to the end user's needs as well as the detrimental effects that each tuning concern can have on the environment and/or turbine performance. The relative importance of each potential dominant tuning concern can be different with each end user, and for each combustor arrangement. For example, some combustion systems will demonstrate an extreme sensitivity to combustor dynamics, such that normal daily operational parameter variations can cause a normally benign dynamics tuning concern to become catastrophic in a very short amount of time. In this case, one or both of the dominant dynamics tuning concerns (Class 1 and Class 2) may be elevated to Priority 1 (Most Important). By way of example in FIG. 7, combustor blowout is listed as the most important Dominant Tuning Concern 144. This ranking is used to determine the dominant tuning concern in the event that there are multiple alarms with equal levels of severity. This ranking of Dominant Tuning Concerns 144, from most to least important, provides the overall framework where the specific Boolean Logic Hierarchy 148 is created. For example, assuming Class 1 and Class 2 δP's obey generally monotonic behavior relative to perturbations in system operational parameters, a High-High “HH” Class 2 δP's alarm may be more significant than High “H” Class 1 δP's alarm. Additionally, in the example given in FIG. 8 for the Boolean Logic Hierarchy 148, High “H” NOx emissions is more significant than High “H” Class 2 dynamics. This means that if both High “H” NOx and High “H” Class 2 dynamics are both “in alarm” (Logic=True), in the absence of other alarms being “True”, the autotuning system will tune for High “H” NOx because it is the dominant tuning concern. Finally, it can be seen that Blowout is ranked above NOx Emissions and both are ranked above Class 1 δP's. Thus, if there were high “H” alarms returned for all three categories, Blowout would be the dominant tuning concern, followed by NOx Emissions and then Class 1 δP's. This Boolean Logic Hierarchy 148 will be what is compared to the “True” alarms 130 returned by comparing the allowable tuning limits 124 to the operational data 120, 122 as set forth above with respect to FIG. 5.

All “True” tuning alarms 130 are provided as ranked by severity (e.g. HHH above HH, etc.). The “True” tuning alarms 130 are then compared with the hard-coded Boolean Logic Hierarchy 148, in step 150 to determine which tuning will become the “True” Dominant Tuning Concern 106. This one “True” Dominant Tuning Concern 106 is now passed into the remainder of the autotuning algorithm, as detailed in FIG. 2, as the Dominant Tuning Concern 106 to be mitigated by operational changes.

Thus the tuning controller 10 may be configured to optimize the mechanical life of a Heat Recovery Steam Generator (HRSG) through the manipulation of the gas turbine exhaust temperature (turbine fuel air (f/a) ratio) when key HRSG operational characteristics indicate insufficient design margin against over-temperature (at steam outlet conditions) and/or over-attemperation (at intra-stage desuperheater). The HRSG will have sensors for measuring operational parameters of the boiler, and the turbine having sensor means for measuring operational parameters of the turbine, as discussed above. The HRSG operational parameters include high pressure and/or hot reheat steam outlet temperatures and/or high pressure and/or hot reheat intra-stage desuperheater outlet temperatures and pressures. The turbine operational parameters include combustor dynamics and turbine exhaust emissions. Using the logic applied above with respect to alarm levels, the turbine controller will adjust various operational control elements, such as fuel distribution and/or fuel-to-air (f/a) ratio, as needed.

The control system for optimizing HRSG life is set forth above in FIG. 1 and (optionally) relies on the turbine controller 10 communicating through the DCS 20 to the sensor means and the control means listed above to control the operational control elements of the turbine. In order to maximize HRSG life in light of other potential operational priorities, a user will select operational priorities for HRSG and/or other turbine operation, selected from the group comprising optimum NOx emissions, optimum power output, optimum combustor dynamics, optimum HRSG life, and/or optimum fuel blend ratio (ratio of non-pipeline quality gas to pipeline quality gas). The below examples will be provided for instances where the Optimum HRSG Life 19 is selected in the control panel shown in FIG. 3, such that Optimum HRSG Life is an operating priority, potentially in addition to other selected priorities.

During operation, the turbine controller will receive operational data from the gas turbine sensor means and the HRSG sensor means. The operational data will be compared to stored operational standards, based on the selected operational priorities. Using this comparison, the turbine controller will determining if both the HRSG and gas turbine operation conform to the operational standards.

To the extent that either the HRSG or gas turbine operational parameters are not within allowable limits, the tuning controller 10 will determine the dominant tuning criteria for non-conforming operation of the HRSG and/or the gas turbine, based on the preset operational priorities. With the dominant tuning criteria determined, the turbine controller 10 will communicate with the selected operational control elements to perform a selected adjustment in the operational control element of the gas turbine. The operational control element may be combustor fuel distribution split within the nozzles of the combustor, fuel gas inlet temperature, fuel/air ratio within the turbine, and/or gas fuel blend ratio (fuel composition). The adjustment to the operational control element will be based on the dominant tuning criteria and have a fixed incremental value and defined range, each incremental change input over a set period of time sufficient for the turbine to gain operational stability.

The sensing process will be repeated in open loop fashion, such that the turbine controller will subsequently receive further data regarding the operational parameters from the HRSG and gas turbine sensor means upon passage of a set period of time to determine if an additional incremental change is desired. If additional tuning is required, further incremental adjustments will be made to the operational control element within a defined range. To the extent that the range of available adjustments to a particular control element are exhausted, the tuning controller 10 will select a further operational control element adjustment based on the dominant tuning criteria, the further selected adjustment having a fixed incremental value and defined range, with each incremental adjustment made over a set period of time sufficient for the turbine to gain operational stability. The sensing and adjustment (if needed) process will be continued during the operation of the turbine and HRSG.

In one embodiment, the system can be programmed with stored operational data, such that the mechanical life of an HRSG is optimized in the tuning process by first adjusting the fuel-to-air ratio of the gas turbine in increments to change the HRSG hot gas inlet conditions to provide sufficient design margin in key HRSG operational parameters (i.e. lowering or raising the temperature of the hot gas inlet). The tuning can then continue as may be required as a result of these changes made to the turbine's f/a ratio. For example, the HRSG may be provided with sensor means for measuring operational parameters of the associated boiler, including high pressure and/or hot reheat outlet steam temperatures as well as high pressure and/or hot reheat intra-stage desuperheater outlet temperatures and pressures. The gas turbine having will also have sensor means for measuring operational parameters of the turbine, including stack emissions and combustion dynamics from the turbine and control means for various operational elements of the turbine, including fuel distribution and/or fuel temperature and/or fuel blend ratio and/or fuel-to-air ratio. Optionally, the tuning controller 10, various sensor means and control means may either be connected directly or via a distributed control system (DCS). The control system may also be provided with means for setting operational priorities for turbine operation, selected from the group comprising optimum NOx emissions, optimum power output, optimum combustor dynamics, optimum fuel blend ratio, and/or optimum HRSG life, such as that shown in FIG. 3 discussed above. Using this tuning system, operational priorities are selected, operational parameters are sensed and tuning occurs using the methods discussed herein with respect to optimizing HRSG life and turbine operation, provided that in this instance, f/a ratio is the predetermined first operational control element to be adjusted to optimize HRSG life, while other operational control elements may be adjusted in order to keep the combustion turbine within the allowable limits for each operational parameter.

A method of optimizing the mechanical life of an HRSG through tuning the operation of a gas turbine, is now disclosed using the systems described herein. The method first includes establishing a communication link between the turbine controller 10 and (optionally) the DCS 20 and receiving data from the HRSG and/or gas turbine sensor means regarding the status of various operational parameters of the HRSG and the turbine. The operational parameter values are then compared to set of standard data to determine if adjustment to operational control elements is required in order to bring the operation of the turbine or HRSG into allowable limits. If tuning is needed, the tuning controller will communicate with the selected operational control elements to perform a defined incremental adjustment of the selected control element. The system then receives, at the tuning controller, via the sensor means and DCS operational parameter data regarding the operation of both the HRSG and the turbine from the sensor means and determines if the adjustment conforms turbine operation to a set standard or if a further incremental adjustment is desired.

The sensed data from the HRSG may include steam outlet temperatures and/or steam superheater intra-stage attemperator over-saturation conditions. The operational control element that is adjusted to modify the values of these sensed parameters may be the fuel-to-air ratio of the turbine. Once the HRSG values are within allowable limits, if further tuning is required to bring the operation of the turbine within its allowable limits. This will be done according to the tuning methods described above, preferably without further modification to the f/a ratio, such that the operational control elements of fuel gas temperature, fuel splits or fuel blend ratio.

The tuning of the system may be adapted for method for tuning a premixed combustion system wherein there exists two distinct modes of operation. The turbine being tuned (not shown) may have an outer ring of identical fuel nozzles utilizing an outer nozzle fuel split to modulate the circumferential fuel distribution within these outer nozzles, an inner fuel nozzle which utilizes an inner nozzle fuel split to adjust the fuel-to-air ratio of the inner to outer nozzles. The outer an inner nozzles discussed herein are known to those skilled in the art and not specifically recounted herein. The two distinct modes of operation comprise a “lean” inner nozzle mode whereby the f/a ratio of the inner nozzle is less than the f/a ratio of the outer fuel nozzles, and a “rich” inner nozzle whereby the f/a ratio of the inner nozzle is greater than the f/a ratio of the outer fuel nozzles. The method for tuning a system having these distinct modes comprises selecting, at the tuning controller 10 of a hybrid fuel split schedule for varying modes based on the turbine load. The “lean” center nozzle fuel split schedule will be at higher load conditions and the “rich” fuel split schedule will be used at lower load and turndown conditions, where the turbine is being operated at the lowest level possible in order to maintain operation of the HRS G.

The method may include the steps disclosed above along with making, at the tuning controller 10, a determination of whether the current mode of operation is utilizing either a “lean” or “rich” inner nozzle mode of operation, and selecting the direction of adjustment for Fuel Circuit Split 1 and/or Fuel Circuit Split 2 when a tuning issue exists, depending on which mode of operation is being utilized at the current operating conditions and preset operational parameters stored within the turbine controller.

All of the methods provided above can be conducted using Boolean-logic toggle switches, such as those shown in FIG. 3, to select user-desired optimization criteria. One of the optimization criteria is Optimum HRSG Life, whereby toggling of this switch to a “1” (“TRUE”) allows the tuning controller to improve HRSG mechanical operating margins, such as steam outlet temperature and/or steam superheater intra-stage attemperator saturation temperature margin, through changes in the HRSG inlet conditions via modifications to the gas turbine fuel-to-air ratio. These changes may be made using the methods and systems disclosed above.

A method for tuning a premixed combustion system is also provided whereby there exists an outer ring of fuel nozzles utilizing an outer nozzle fuel split to modulate the circumferential fuel distribution within these outer nozzles, utilizing two modes of operation: a “lean minor circuit 1” subset of the outer nozzles whereby the f/a ratio of this outer fuel nozzle subset is less than the f/a ratio of the remaining outer fuel nozzles, and a “rich minor circuit 1” inner nozzle whereby the f/a ratio of this outer fuel nozzle subset is greater than the f/a ratio of the remaining outer fuel nozzles. The method includes usage of a hybrid fuel split schedule, with a “rich minor circuit 1” fuel split schedule at higher load conditions, and usage to a “lean minor circuit 1” fuel split schedule at lower load and turndown conditions. The method may also include varying other operational control elements, as described herein, in order to bring the operation of the turbine or HRSG into allowable limits.

The method may also include usage of a hybrid fuel split schedule, with a “lean minor circuit 1” fuel split schedule at higher load conditions, and usage to a “rich minor circuit 1” fuel split schedule at lower load and turndown conditions. Further, the method may include making a determination, at the tuning controller 10, if the current mode of operation is utilizing either a “lean minor circuit 1” or “rich minor circuit 1” mode of operation, and adjusting, using operational control elements for fuel splits, the Fuel Circuit Split 1 and/or Fuel Circuit Split 2 in the proper direction, when a tuning issue exists, depending on which mode of operation is being utilized at the current operating conditions.

A method is also provided for tuning a premixed combustion system, using similar systems and steps as described above, whereby there exists one or more annular rings of fuel nozzles (of same or different type, controlled by an circumferential fuel split affecting circumferential distribution of fuel within each fuel nozzle ring). In the current system, it is contemplated that a second family of fuel splits may be available (if more than one annular ring of fuel nozzles exists), which adjusts the relative (radial) amount of fuel to each of the radially concentric fuel nozzle rings (ring 1, ring 2, etc.), utilizing two modes of operation: a “lean minor circuit ring 1” subset of the ring 1 fuel nozzles whereby the f/a ratio of this ring 1 fuel nozzle subset is less than the f/a ratio of the remaining fuel nozzles of ring 1, and a “rich minor circuit ring 1” subset of the ring 1 fuel nozzles whereby the f/a ratio of this outer fuel nozzle subset is greater than the f/a ratio of the remaining fuel nozzles of ring 1. The tuning method comprises, use of a hybrid fuel split schedule, with a “lean minor circuit ring 1” fuel split schedule at higher load conditions, usage of a “rich minor circuit ring 1” fuel split schedule at lower load and turndown conditions, and similar usage of “rich” and “lean” fuel split schedules, one at high loads and the other at lower load/turndown conditions, for each of the remaining fuel nozzle rings of the combustion system. Each of the fuel schedules may be pre-programmed into the tuning controller 10 and selected based on sensed operational parameters of the system.

The method may also be modified, depending on operational priorities and user input to the tuning controller 10, to include usage of a hybrid fuel split schedule, with a “rich minor circuit ring 1” fuel split schedule at higher load conditions, usage to a “lean minor circuit ring 1” fuel split schedule at lower load and turndown conditions, and similar usage of “rich” and “lean” fuel split schedules, one at high loads and the other at lower load/turndown conditions, for each of the remaining fuel nozzle rings of the combustion system.

A method is also provided for tuning a premixed combustion system, such as that disclosed above, whereby there exists one or more annular rings of fuel nozzles (of same or different type, controlled by an circumferential fuel split affecting circumferential distribution of fuel within each fuel nozzle ring), whereby a second family of fuel splits may be available (if more than one annular ring of fuel nozzles exists) which adjusts the relative (radial) amount of fuel to each of the radially concentric fuel nozzle rings (ring 1, ring 2, etc.), utilizing two modes of operation: a “lean minor circuit ring 1” subset of the ring 1 fuel nozzles whereby the f/a ratio of this ring 1 fuel nozzle subset is less than the f/a ratio of the remaining fuel nozzles of ring 1, and a “rich minor circuit ring 1” subset of the ring 1 fuel nozzles whereby the f/a ratio of this outer fuel nozzle subset is greater than the f/a ratio of the remaining fuel nozzles of ring 1. The method first comprises the step of determining if the current mode of operation is utilizing either a “lean minor circuit ring 1” or “rich minor circuit ring 1” mode of operation, making a similar determination of the current mode of operation, either “rich” or “lean” minor fuel circuit operation, for each of the remaining fuel nozzle rings of the combustion system. Once these determinations are made, the method comprises the step of adjusting, via the tuning controller 10 and selected operational control element, Fuel Circuit Split 1 and/or Fuel Circuit Split 2 in the proper direction, when a tuning issue exists. The direction of adjustment is determined based on which mode of operation is being utilized at the current operating conditions.

FIGS. 9-12 provide exemplary visual representations of the autotuning system interface depicting how the Boolean Logic Hierarchy works in practice. FIG. 9 shows the alarms returned in connection with the example set forth above with respect to FIG. 8. Namely, alarms are returned for Class 2 δP's at the levels of H 162, HH 164 and HHH 166. In addition, alarms for NOx 168 and Class 1 δP's 170 are returned at the H level. Since more extreme levels trump conflicts of different alarms at the same level, the HHH Class 2 δP's is the priority and therefore the dominant tuning concern 172.

FIGS. 10-12 show various further examples of the dominant tuning concern for different “True” alarm levels under the user defined hierarchy 144 of FIG. 8. FIG. 10 shows high pressure steam at maximum operating temperature and the high pressure steam desuperheater at saturation conditions (placing water into the steam pipe), with no other alarms active. Thus, HRSG Mechanical Life Optimization is the dominant tuning concern. FIG. 11 shows a Class 2δP's at an H level, with NOx at both an H and HH condition, thus making High NOx as the dominant tuning concern. Finally, FIG. 12 shows both Class 1 δP's and Class 2 δP's at the H level. Referring to the user ranking of dominant tuning issues 144 in FIG. 8, Class 1 δP's is ranked as a priority above Class 2 δP's and thus, although the severity of the alarms is equal, Class 1 δP's becomes the dominant tuning concern.

In FIGS. 13-16, there is shown various examples of the operational results of a tuning operation of a tuning controller of the present disclosure based on operational data from a running turbine system. In FIG. 13, the dominant tuning concern is high Class 2 δP's, and a change in the combustor fuel split E1 is made in reaction to a high Class 2 δP's alarm generated when the combustor dynamics moves outside of the set operational priorities for optimum dynamics. The actual combustor dynamics data received by the turbine controller 10 from, for example, the CDMS 50 is designated as 200 in the graph. The moving average for the combustor dynamics is identified in the graph as 202. When the combustor dynamics exceed the dynamics alarm limit value 204 for a set period of time TA an alarm goes off within the tuning controller. This alarm causes the first event E1 and a resulting incremental adjustment in the combustor fuel split tuning parameter 206. As illustrated, the incremental increase in the fuel split causes a corresponding drop in the combustor dynamics 200, with the average combustor dynamics 202 dropping below the dynamics alarm limit 204. As time continues, the tuning is held by the tuning controller and the average combustor dynamics 202 maintains its operational position below the dynamics limit 204. Thus, no further adjustments necessary or alarms issued.

In FIG. 14, the tuning criteria is High NOx emissions. As NOx emissions data 210 is received from the tuning controller, an alarm is generated after the passage of time TA. The alarm is caused by the NOx emissions 210 exceeding the operational standard or tuning limit 212. The alarm activates a first event E1 resulting in an incremental increase in the fuel split 214. After a period of time TB from the first event E1, the NOx alarm is still activated due to the NOx emissions 210 exceeding the preset tuning limit 212. This continued alarm after time TB causes a second event E2 and a second incremental increase in the fuel split value 214. This second increase is equal in magnitude to the first incremental increase. The second event E2 causes the NOx emissions level 210 to drop below the preset limit 212 within the review time period and halts the alarm. As the NOx emissions 210 remains below the limit 212, the fuel split 214 tuning is held and the operation of the turbine continues with the defined operational parameters.

In FIG. 15, the tuning criteria is Blowout, with the alarm created by a low NOx reading received by tuning controller. As shown, the NOx tuning limit 220 is defined. Upon passage of the set time period TA from receiving NOx level data 222, the alarm is generated and a first event E1 occurs. At the first event E1, the fuel split level 224 is incrementally adjusted downward. After a set passage of time TB from event E1 additional NOx emissions data 222 is received and compared to the preset alarm level 220. Because the NOx is still below the alarm level 220, a second event E2 occurs resulting in a further incremental reduction in the fuel split value 224. A further passage of time TC from event E2 occurs and additional data is received. Again, the NOx data 222 is low, maintaining the alarm and resulting in a further event E3. At event E3, the fuel split value 224 is again reduced by the same incremental amount. This third incremental adjustment results in the NOx emissions 222 rising above the preset limit 220 and results in removal of the alarm. The fuel split 224 tuning value set after event E3 is held in place by the tuning controller 10.

In FIG. 16, the tuning criteria is again Blowout, whereby the NOx emissions data 230 received by the tuning controller 10 is again tracking along the lower emissions limit 232. At the first tuning event E1, the fuel split value 234 is incrementally dropped to result in a corresponding increase in the NOx emissions 230 over the lower limit 232. After this first incremental adjustment, the NOx emissions for a period of time holds above the limit 232 and then begins to again fall. At the second tuning event E2, the fuel split value 234 is again adjusted by the designated fixed incremental value. This second adjustment then places the fuel split value 234 at its defined minimum within the preset range of allowable values (determined as a hard coded limit within the tuning controller 10). Because this limit is reached, the tuning operation moves to the next operational parameter, which is normally the second fuel circuit adjustment. In the example provided, this second circuit value (not shown) is already at its set maximum/minimum and is therefore not adjusted. Thus, the tuning operation moves on to the next operational parameter, load control curves 236. As shown, at event E2 an incremental adjustment is made in the load control curve value 236. The increase in the load control curve value 236 results in a corresponding increase in the NOx emission 230 to a value above the minimum 232 and removes the alarm. Upon removal of the alarm, the tuning settings are held and no further adjustments are made. The tuning controller 10 then proceeds to receive data from the sensor means, through the DCS, and continues to make comparisons with the set operational standards (including the minimum NOx emissions limit EL).

The present invention has been described and illustrated with respect to a number of exemplary embodiments thereof. It should be understood by those skilled in the art from the foregoing that various other changes, omissions and additions may be made therein, without departing from the spirit and scope of the present invention, with the scope of the present invention being described by the foregoing claims.

Claims

1. A tuning system for optimizing the mechanical life of a heat recovery steam generator, the heat recovery steam generator being operated in connection with a combustion turbine, the tuning system comprising:

a turbine controller;
sensor means for sensing the operational parameters of a turbine and heat recovery steam generator; and
control means for controlling various operational control elements,
wherein the turbine controller is adapted to tune the operation of the gas turbine in accordance with the following steps: selecting operational priorities for at least one of the heat recovery steam generator or turbine operation, whereby each selected operational priority will determine operational standards for the heat recovery steam generator and turbine, receiving operational parameter data for the operation of the turbine and the heat recovery steam generator from the sensor means, comparing the operational data to stored operational standards based on the selected operational priorities to determine if both heat recovery steam generator and turbine operation conform to the operational standards, determining the dominant tuning criteria for non-conforming operation of the heat recovery steam generator and turbine, based on the preset operational priorities, communicating with the control means to perform a selected adjustment in a first operational control element of the gas turbine, receiving operational data from the sensor means upon passage of a set period of time to determine if an additional incremental change is desired, and making further adjustments to the selected first operational control element, selecting a further operational parameter adjustment, different than the first selected operational control element, and receiving operational data from the sensor means upon passage of a set period of time to determine if an additional incremental change is desired.

2. The system of claim 1, further comprising a distributed control system, whereby the tuning controller communicates with the sensor means and the control means using the distributed control system.

3. The system of claim 1, wherein the operational priorities are selected from the group comprising optimum NOx emissions, optimum power output, optimum combustor dynamics, optimum heat recovery steam generator life, and optimum fuel blend ratio.

4. The system of claim 3, wherein the optimum fuel blend ratio comprises the ratio of non-pipeline quality gas to pipeline quality gas.

5. The system of claim 1, wherein, the selected operational control element adjustment based on the dominant tuning criteria, the selected adjustment having a fixed incremental value and defined range, each incremental change input over a set period of time sufficient for the turbine to gain operational stability.

6. The system of claim 1, wherein the adjustments in the operational control elements of the gas turbine are selected from the group comprising combustor fuel distribution split within the nozzles of the combustor, fuel gas inlet temperature, fuel/air ratio within the turbine, and gas fuel blend ratio (fuel composition).

7. The system of claim 1, wherein the operational priorities comprise optimum heat recovery steam generator life, and wherein adjustment to the fuel-to-air ratio of the turbine is selected as the first operational control element to be adjusted when the selected operational priority is optimum heat recovery steam generator life.

8. The system of claim 1, wherein the tuning controller is adapted to optimizing the mechanical life of the heat recovery steam generator by first adjusting the fuel-to-air ratio operational control element prior to making any tuning adjustments based on remaining operational priorities.

9. The system of claim 8, wherein, after adjustment of the fuel-to-air ratio operational control element, the turbine controller subsequently tunes additional control elements in response to changes in operational parameters of the turbine occurring as the result of adjustment of the fuel-to-air ratio operational control element.

10. The system of claim 1, wherein the heat recovery steam generator has operational parameters are selected from the group consisting of high pressure outlet steam temperatures, hot reheat steam temperatures, high pressure intra-stage desuperheater outlet temperatures and pressures, and hot reheat intra-stage desuperheater outlet temperatures and pressures.

11. The system of claim 1, wherein the turbine has operational parameters selected from the group consisting of turbine stack emissions and combustion dynamics.

12. A method of optimizing the mechanical life of a heat recovery steam generator through tuning the operation of a gas turbine, the method comprising:

providing sensor means for sensing the operational parameters of the heat recovery steam generator;
providing control means for controlling operational control elements of the turbine, wherein the control means adjust selected control elements in response to control signals from the tuning controller;
providing a tuning controller for receiving data regarding the operational parameters from the sensor means and sending control signals to the control means;
establishing a communication link between the tuning controller, the control means and the sensor means;
sensing data regarding operational parameters of the heat recovery steam generator and the turbine and transmitting the sensed data to the turbine controller;
receiving the sensed operational parameter data at the turbine controller and comparing the sensed operational parameter data to stored operational data stored in the turbine controller to determine if adjustment to an operational control element is necessary to improve operating parameters of the turbine or heat recovery steam generator, wherein the preset operational parameter levels are based on operational priorities of the turbine;
communicating, from the turbine controller to the control means, control signals perform a defined incremental adjustment of a first selected operational control element,
after a preset period of time from the adjustment of the first selected operational control element, sensing data regarding operational parameters and transmitting the sensed data to the turbine controller and comparing the sensed operational data to the preset operational parameter levels determine if further adjustments within the operational control means are required,
determining if the first operational control element is able to receive further adjustments and communicating, from the turbine controller to the control means, control signals perform a defined incremental adjustment of a second selected operational control element.

13. The method of claim 12, further comprising the step of selecting operational priorities of the turbine and heat recovery steam generator.

14. The method of claim 12, wherein the first selected control element to be adjusted is the fuel-to-air ratio of the turbine, wherein the adjustment to the fuel-to-air ratio is done in response to operational parameters of the heat recovery steam generator being out of allowable limits when compared to the stored operational data.

15. A method for tuning a premixed combustion system of a combustion turbine, the turbine comprising at least one combustor having an outer ring of identical fuel nozzles and an inner fuel nozzle which utilizes an inner nozzle fuel split to adjust the fuel-to-air ratio of the inner to outer nozzles, the method comprising:

providing a turbine controller programmed to operate the premixed combustion system according to at least two distinct modes of operation, the distinct modes comprising a lean inner nozzle mode whereby the fuel-to-air ratio of the inner nozzle is less than the fuel-to-air ratio of the outer fuel nozzles, and a rich inner nozzle mode whereby the fuel-to-air ratio of the inner nozzle is greater than the fuel-to-air ratio of the outer fuel nozzles,
sensing the operating conditions of the turbine, wherein the sensed conditions include high load, low load and turndown; and
operating the premixed combustion system using both the lean inner nozzle mode and the rich inner nozzle mode according to the operating condition of the turbine; wherein modifying the operational mode of the turbine from lean inner nozzle mode to rich inner nozzle mode is done by adjusting the fuel splits of the turbine.

16. The method of claim 15, wherein the premixed combustion system is operated at a lean inner nozzle mode during high load conditions and the premixed combustion system is operated at rich inner nozzle mode during low load and turndown conditions.

17. The method of claim 15, wherein the premixed combustion system is operated at a rich inner nozzle mode during high load conditions and the premixed combustion system is operated at lean inner nozzle mode during low load and turndown conditions.

Referenced Cited
U.S. Patent Documents
3842597 October 1974 Ehrich
3866109 February 1975 Reed et al.
3875380 April 1975 Rankin
3898439 August 1975 Reed et al.
3919623 November 1975 Reuther
3924140 December 1975 Yannone
4010605 March 8, 1977 Uram
4027145 May 31, 1977 McDonald et al.
4028884 June 14, 1977 Martz et al.
4031404 June 21, 1977 Martz et al.
4039804 August 2, 1977 Reed et al.
4039846 August 2, 1977 Vance
4051669 October 4, 1977 Yannone et al.
4115998 September 26, 1978 Gilbert et al.
4195231 March 25, 1980 Reed et al.
4201923 May 6, 1980 Reed et al.
4208591 June 17, 1980 Yannone et al.
4278064 July 14, 1981 Regueiro
4280060 July 21, 1981 Kure-Jensen et al.
4283634 August 11, 1981 Yannone et al.
4305129 December 8, 1981 Yannone et al.
4308463 December 29, 1981 Giras et al.
4314441 February 9, 1982 Yannone et al.
4319320 March 9, 1982 Sato et al.
4333310 June 8, 1982 Uram
4414540 November 8, 1983 Dickenson
4445180 April 24, 1984 Davis et al.
4455614 June 19, 1984 Martz et al.
4716858 January 5, 1988 Bartels
4735052 April 5, 1988 Maeda et al.
4761948 August 9, 1988 Sood et al.
4811555 March 14, 1989 Bell
4845940 July 11, 1989 Beer
4893467 January 16, 1990 Woodson
4930305 June 5, 1990 Bell
4936088 June 26, 1990 Bell
5022849 June 11, 1991 Yoshii et al.
5024055 June 18, 1991 Kirikami et al.
5237939 August 24, 1993 Spokoyny et al.
5307619 May 3, 1994 McCarty et al.
5319931 June 14, 1994 Beebe et al.
5319936 June 14, 1994 Ikeda et al.
5339635 August 23, 1994 Iwai et al.
5349812 September 27, 1994 Taniguchi et al.
5365732 November 22, 1994 Correa
5367470 November 22, 1994 Lang
5423175 June 13, 1995 Beebe et al.
5450724 September 19, 1995 Kesseli et al.
5480298 January 2, 1996 Brown
5487265 January 30, 1996 Rajamani et al.
5490377 February 13, 1996 Janes
5491970 February 20, 1996 Davis, Jr. et al.
5517424 May 14, 1996 Marcelle et al.
5533329 July 9, 1996 Ohyama et al.
5551228 September 3, 1996 Mick et al.
5564270 October 15, 1996 Kesseli et al.
5609655 March 11, 1997 Kesseli et al.
5636507 June 10, 1997 Rajamani et al.
5661969 September 2, 1997 Beebe et al.
5706643 January 13, 1998 Snyder et al.
5719791 February 17, 1998 Neumeier et al.
5722230 March 3, 1998 Cohen et al.
5729968 March 24, 1998 Cohen et al.
5784300 July 21, 1998 Neumeier et al.
5790420 August 4, 1998 Lang
5791889 August 11, 1998 Gemmen et al.
5794446 August 18, 1998 Earley et al.
5826429 October 27, 1998 Beebe et al.
5845230 December 1, 1998 Lamberson
5847353 December 8, 1998 Titus et al.
5867977 February 9, 1999 Zachary et al.
5878566 March 9, 1999 Endo et al.
5896736 April 27, 1999 Rajamani
5924275 July 20, 1999 Cohen et al.
5930990 August 3, 1999 Zachary et al.
5943866 August 31, 1999 Lovett et al.
6055808 May 2, 2000 Poola et al.
6066825 May 23, 2000 Titus et al.
6071114 June 6, 2000 Cusack et al.
6082092 July 4, 2000 Vandervort
6092362 July 25, 2000 Nagafuchi et al.
6125625 October 3, 2000 Lipinski et al.
6138081 October 24, 2000 Olejack et al.
6145297 November 14, 2000 Nagafuchi et al.
6164055 December 26, 2000 Lovett et al.
6195607 February 27, 2001 Rajamani et al.
6196000 March 6, 2001 Fassbender
6202401 March 20, 2001 Seume et al.
6205765 March 27, 2001 Iasillo et al.
6250063 June 26, 2001 Davis, Jr. et al.
6269299 July 31, 2001 Blotenberg
6287111 September 11, 2001 Gensler
6293105 September 25, 2001 Claesson et al.
6298718 October 9, 2001 Wang
6324827 December 4, 2001 Basu et al.
6338240 January 15, 2002 Endo et al.
6341519 January 29, 2002 Khesin et al.
6343251 January 29, 2002 Herron et al.
6354071 March 12, 2002 Tegel et al.
6363330 March 26, 2002 Alag et al.
6389330 May 14, 2002 Khesin
6397602 June 4, 2002 Vandervort et al.
6405523 June 18, 2002 Foust et al.
6408611 June 25, 2002 Keller et al.
6412271 July 2, 2002 Maker et al.
6418726 July 16, 2002 Foust et al.
6460339 October 8, 2002 Nishida et al.
6460341 October 8, 2002 Gutmark et al.
6461144 October 8, 2002 Gutmark et al.
6464489 October 15, 2002 Gutmark et al.
6466859 October 15, 2002 Fujime
6480810 November 12, 2002 Cardella et al.
6484489 November 26, 2002 Foust et al.
6522991 February 18, 2003 Banaszuk et al.
6522994 February 18, 2003 Lang
6529849 March 4, 2003 Umezawa et al.
6556956 April 29, 2003 Hunt
6560563 May 6, 2003 Lang
6568166 May 27, 2003 Jay et al.
6584429 June 24, 2003 Lang
6598383 July 29, 2003 Vandervort et al.
6612112 September 2, 2003 Gilbreth et al.
6616901 September 9, 2003 Lagana et al.
6640544 November 4, 2003 Suenaga et al.
6651035 November 18, 2003 Lang
6657332 December 2, 2003 Balas
6672071 January 6, 2004 Woltmann
6691054 February 10, 2004 Lang
6694900 February 24, 2004 Lissianski et al.
6704620 March 9, 2004 Kutzner et al.
6714877 March 30, 2004 Lang
6721631 April 13, 2004 Shimizu et al.
6721649 April 13, 2004 Knott et al.
6722135 April 20, 2004 Davis, Jr. et al.
6725665 April 27, 2004 Tuschy et al.
6742341 June 1, 2004 Ryan et al.
6745152 June 1, 2004 Lang
6757619 June 29, 2004 Zison et al.
6760659 July 6, 2004 Cowen
6760689 July 6, 2004 Follin et al.
6766224 July 20, 2004 Tanaka
6772583 August 10, 2004 Bland
6789000 September 7, 2004 Munson, Jr.
6799146 September 28, 2004 Lang
6810358 October 26, 2004 Lang et al.
6810655 November 2, 2004 Davis, Jr. et al.
6834226 December 21, 2004 Hartzheim
6839613 January 4, 2005 McCarthy et al.
6840046 January 11, 2005 Paschereit et al.
6845300 January 18, 2005 Haghgooie et al.
6862889 March 8, 2005 Held et al.
6865889 March 15, 2005 Mancini et al.
6868368 March 15, 2005 Lang
6871501 March 29, 2005 Bibler et al.
6873933 March 29, 2005 Lang
6877307 April 12, 2005 Ryan et al.
6880325 April 19, 2005 Aoyama
6883301 April 26, 2005 Woltmann
6898488 May 24, 2005 Kusaka et al.
6910335 June 28, 2005 Viteri et al.
6912855 July 5, 2005 Bescherer et al.
6912856 July 5, 2005 Morgan et al.
6912889 July 5, 2005 Staphanos et al.
6918253 July 19, 2005 Fassbender
6920761 July 26, 2005 Laper
6931853 August 23, 2005 Dawson
6941217 September 6, 2005 Munson, Jr.
6952639 October 4, 2005 Kumar et al.
6952642 October 4, 2005 Cowen
6955039 October 18, 2005 Nomura et al.
6968693 November 29, 2005 Colibaba-Evulet et al.
6973376 December 6, 2005 Kusaka et al.
6973790 December 13, 2005 Suenaga et al.
6973791 December 13, 2005 Handelsman et al.
6976351 December 20, 2005 Catharine et al.
6986254 January 17, 2006 Stuttaford et al.
6989693 January 24, 2006 Kuo et al.
6990432 January 24, 2006 McCarthy et al.
6996991 February 14, 2006 Gadde et al.
7006898 February 28, 2006 Barbir et al.
7007487 March 7, 2006 Belokon et al.
7039555 May 2, 2006 Lang
7047747 May 23, 2006 Tanaka
7050943 May 23, 2006 Kauffman et al.
7059135 June 13, 2006 Held et al.
7062389 June 13, 2006 Johnson et al.
7065471 June 20, 2006 Gotoh et al.
7065472 June 20, 2006 Hayashi et al.
7089746 August 15, 2006 Lieuwen et al.
7100357 September 5, 2006 Morgan et al.
7107773 September 19, 2006 Little
7111463 September 26, 2006 Sprouse et al.
7127329 October 24, 2006 Kusaka et al.
7127898 October 31, 2006 Healy
7143572 December 5, 2006 Ooka et al.
7161678 January 9, 2007 Schultz
7162875 January 16, 2007 Fletcher et al.
7177728 February 13, 2007 Gardner
7181320 February 20, 2007 Whiffen et al.
7181321 February 20, 2007 Schlicker et al.
7181916 February 27, 2007 Ziminsky et al.
7185494 March 6, 2007 Ziminsky et al.
7188019 March 6, 2007 Nomura et al.
7188465 March 13, 2007 Kothnur et al.
7190149 March 13, 2007 Huff et al.
7204133 April 17, 2007 Benson et al.
7210297 May 1, 2007 Shah et al
7216486 May 15, 2007 Doebbeling et al.
7219040 May 15, 2007 Renou et al.
7234305 June 26, 2007 Nomura et al.
7237385 July 3, 2007 Carrea
7246002 July 17, 2007 Healy et al.
7246024 July 17, 2007 Muramatsu et al.
7249462 July 31, 2007 Aumont et al.
7260466 August 21, 2007 Fujii
7260935 August 28, 2007 Colibaba-Evulet et al.
7260937 August 28, 2007 Kothnur et al.
7269939 September 18, 2007 Kothnur et al.
7269952 September 18, 2007 Arar et al.
7269953 September 18, 2007 Gadde et al.
7275025 September 25, 2007 Chan et al.
7278266 October 9, 2007 Taware et al.
7284378 October 23, 2007 Amond, III et al.
7288921 October 30, 2007 Huff et al.
7299279 November 20, 2007 Sadaghiany
7302334 November 27, 2007 Hook et al.
7320213 January 22, 2008 Shah et al.
7334413 February 26, 2008 Myhre
7349765 March 25, 2008 Reaume et al.
7353084 April 1, 2008 Schaper et al.
7356383 April 8, 2008 Pechtl et al.
7368827 May 6, 2008 Kulkarni et al.
7369932 May 6, 2008 Kim et al.
7377036 May 27, 2008 Johnson et al.
7385300 June 10, 2008 Huff et al.
7389151 June 17, 2008 Badami et al.
7389643 June 24, 2008 Simons et al.
7406820 August 5, 2008 Critchley et al.
7409855 August 12, 2008 Flint
7415779 August 26, 2008 St. Louis et al.
7435080 October 14, 2008 Joklik et al.
7437871 October 21, 2008 Cook
7441398 October 28, 2008 Ziminsky et al.
7441448 October 28, 2008 Volponi
7451601 November 18, 2008 Taware et al.
7456517 November 25, 2008 Campbell et al.
7457688 November 25, 2008 Szepek et al.
7457710 November 25, 2008 Schuermans et al.
7461509 December 9, 2008 Mick et al.
7471996 December 30, 2008 Bartel
7474080 January 6, 2009 Huff et al.
7478525 January 20, 2009 Iya et al.
7481100 January 27, 2009 Ponziani et al.
7484369 February 3, 2009 Myhre
7486864 February 3, 2009 Diatzikis
7487642 February 10, 2009 Joshi et al.
7489835 February 10, 2009 Xia et al.
7490596 February 17, 2009 Yasui et al.
7493207 February 17, 2009 Yasui et al.
7493752 February 24, 2009 Horswill et al.
7503177 March 17, 2009 Bland et al.
7509810 March 31, 2009 Smith et al.
7512476 March 31, 2009 Rosi et al.
7513099 April 7, 2009 Nuding et al.
7530216 May 12, 2009 Tsuzuki et al.
7530260 May 12, 2009 Dooley
7534033 May 19, 2009 Prinz et al.
7536992 May 26, 2009 Wieshuber et al.
7546741 June 16, 2009 Sasao et al.
7562532 July 21, 2009 Diaz et al.
7565238 July 21, 2009 Nakagawa et al.
7565792 July 28, 2009 Tanaka et al.
7565805 July 28, 2009 Steber et al.
7568349 August 4, 2009 Hadley
7571045 August 4, 2009 Muramatsu et al.
7577549 August 18, 2009 Osborn et al.
7582359 September 1, 2009 Sabol et al.
7584617 September 8, 2009 Bland et al.
7591135 September 22, 2009 Stewart
7600369 October 13, 2009 Tanaka et al.
7610745 November 3, 2009 Fujii et al.
7610746 November 3, 2009 Fujii et al.
7617686 November 17, 2009 Lilley et al.
7617687 November 17, 2009 West et al.
7620461 November 17, 2009 Frederick et al.
7623999 November 24, 2009 Clayton
7628062 December 8, 2009 Healy et al.
7628078 December 8, 2009 Matsui et al.
7630820 December 8, 2009 Sims et al.
7632059 December 15, 2009 Tisenchek et al.
7640725 January 5, 2010 Bland et al.
7640793 January 5, 2010 McCall et al.
7644574 January 12, 2010 Feiz
7644577 January 12, 2010 Linna et al.
7647778 January 19, 2010 Zewde et al.
7650050 January 19, 2010 Haffner et al.
7665670 February 23, 2010 Ahmed
7677075 March 16, 2010 Nies
7681440 March 23, 2010 Thomassin et al.
7684880 March 23, 2010 Bach
7690204 April 6, 2010 Drnevich et al.
7692324 April 6, 2010 Malakhova et al.
7693147 April 6, 2010 Williams et al.
7693643 April 6, 2010 Kim et al.
7698030 April 13, 2010 Martin
7698897 April 20, 2010 Rowe et al.
7702447 April 20, 2010 Volponi
7703288 April 27, 2010 Rogers
7707833 May 4, 2010 Bland et al.
7712313 May 11, 2010 Kojovic et al.
7730726 June 8, 2010 Asti et al.
7751943 July 6, 2010 Bollhalder et al.
7756626 July 13, 2010 Fujii et al.
7757491 July 20, 2010 Hessler
7765856 August 3, 2010 Wilbraham
7769507 August 3, 2010 Volponi et al.
7775052 August 17, 2010 Cornwell et al.
7788014 August 31, 2010 Volponi
7797113 September 14, 2010 Yoshida et al.
7805922 October 5, 2010 Bland
7818970 October 26, 2010 Price et al.
7822512 October 26, 2010 Thatcher et al.
7822576 October 26, 2010 Flint et al.
7823388 November 2, 2010 Murakami
7826954 November 2, 2010 Muramatsu et al.
7832210 November 16, 2010 Fecamp et al.
7836676 November 23, 2010 Futa, Jr. et al.
7837429 November 23, 2010 Zhang et al.
7840336 November 23, 2010 Muramatsu et al.
7841180 November 30, 2010 Kraemer et al.
7841317 November 30, 2010 Williams et al.
7853433 December 14, 2010 He et al.
7853441 December 14, 2010 Volponi et al.
7861578 January 4, 2011 Adibhatla et al.
7871237 January 18, 2011 Bunce et al.
7878004 February 1, 2011 Davies et al.
7886875 February 15, 2011 Shevchencko et al.
7895821 March 1, 2011 Annigeri et al.
7908072 March 15, 2011 Tonno et al.
7927095 April 19, 2011 Chorpening et al.
7942038 May 17, 2011 Ziminsky et al.
7945523 May 17, 2011 Hofmann et al.
7950216 May 31, 2011 Dooley et al.
7957845 June 7, 2011 Chen
7966100 June 21, 2011 Beekhuis
7966801 June 28, 2011 Umeh et al.
7966802 June 28, 2011 Szepek et al.
7966804 June 28, 2011 Snow
7966834 June 28, 2011 Myhre
7966995 June 28, 2011 Futa, Jr. et al.
7970570 June 28, 2011 Lynch et al.
7975533 July 12, 2011 Andrie
7980082 July 19, 2011 Ziminsky et al.
7983829 July 19, 2011 Muramatsu et al.
7997083 August 16, 2011 Meadows et al.
8001761 August 23, 2011 Myers, Jr. et al.
8005575 August 23, 2011 Kirchhof
8014929 September 6, 2011 Page et al.
8015791 September 13, 2011 Finkbeiner
8015792 September 13, 2011 Raver
8018590 September 13, 2011 Davis, Jr. et al.
8024934 September 27, 2011 Abreu et al.
8024964 September 27, 2011 Healy et al.
8028512 October 4, 2011 Mendoza et al.
8033117 October 11, 2011 Ziminsky et al.
8037688 October 18, 2011 Hagen et al.
8042340 October 25, 2011 Ma et al.
8056062 November 8, 2011 Bowers et al.
8056317 November 15, 2011 Feiz
8061118 November 22, 2011 Kothnur et al.
8068997 November 29, 2011 Ling et al.
8099181 January 17, 2012 Sterzing et al.
8145403 March 27, 2012 Fuller et al.
8417433 April 9, 2013 Gauthier
9097185 August 4, 2015 Demougeot
20020084702 July 4, 2002 Balas
20020099474 July 25, 2002 Khesin
20020107614 August 8, 2002 Tanaka
20020142257 October 3, 2002 Eroglu et al.
20020198629 December 26, 2002 Ellis
20030009401 January 9, 2003 Ellis
20030018394 January 23, 2003 McCarthy et al.
20030036820 February 20, 2003 Yellepeddy et al.
20030037550 February 27, 2003 Fassbender
20030056517 March 27, 2003 Brushwood et al.
20030093184 May 15, 2003 Tanaka
20030120444 June 26, 2003 Zison et al.
20030144787 July 31, 2003 Davis, Jr. et al.
20030211432 November 13, 2003 Gutmark et al.
20030233831 December 25, 2003 Suenaga et al.
20040011051 January 22, 2004 Ryan et al.
20040025512 February 12, 2004 Davis, Jr. et al.
20040088060 May 6, 2004 Renou et al.
20040102872 May 27, 2004 Schick et al.
20040103068 May 27, 2004 Eker et al.
20040128111 July 1, 2004 Lang
20040128266 July 1, 2004 Yellepeddy et al.
20040159142 August 19, 2004 Knott et al.
20040191914 September 30, 2004 Widmer et al.
20040194468 October 7, 2004 Ryan et al.
20040197239 October 7, 2004 Mirkovic et al.
20040249515 December 9, 2004 Johnson et al.
20040255595 December 23, 2004 Morgan et al.
20050011179 January 20, 2005 Ooka et al.
20050021710 January 27, 2005 Johnson et al.
20050022499 February 3, 2005 Belokon et al.
20050038570 February 17, 2005 Grauer
20050049775 March 3, 2005 Mooney
20050061004 March 24, 2005 Colibaba-Evulet et al.
20050107941 May 19, 2005 Healy
20050107942 May 19, 2005 Nomura et al.
20050114010 May 26, 2005 Healy et al.
20050143865 June 30, 2005 Gardner
20050144955 July 7, 2005 Handelsman et al.
20050159849 July 21, 2005 Johnson et al.
20050160717 July 28, 2005 Sprouse et al.
20050188745 September 1, 2005 Staphanos et al.
20050203670 September 15, 2005 Kusaka et al.
20050217276 October 6, 2005 Colibaba-Evulet et al.
20050223713 October 13, 2005 Ziminsky et al.
20050247064 November 10, 2005 Lieuwen
20050257514 November 24, 2005 Morgan et al.
20050267642 December 1, 2005 Whiffen et al.
20050268617 December 8, 2005 Amond, III et al.
20050274115 December 15, 2005 Pearce
20050276306 December 15, 2005 Mick et al.
20050278076 December 15, 2005 Barbir et al.
20060040225 February 23, 2006 Garay et al.
20060041368 February 23, 2006 Williams et al.
20060080965 April 20, 2006 Healy
20060106501 May 18, 2006 Gomer et al.
20060137353 June 29, 2006 Lieuwen et al.
20060149423 July 6, 2006 Barnicki et al.
20060178782 August 10, 2006 Pechtl et al.
20060190139 August 24, 2006 Reaume et al.
20060228596 October 12, 2006 Campbell et al.
20060230743 October 19, 2006 Sprouse et al.
20060254279 November 16, 2006 Taware et al.
20060260319 November 23, 2006 Ziminsky et al.
20060288706 December 28, 2006 Ziminsky et al.
20070021899 January 25, 2007 Griffin et al.
20070055392 March 8, 2007 D'Amato et al.
20070067068 March 22, 2007 Havlena et al.
20070074519 April 5, 2007 Hadley
20070084217 April 19, 2007 Nicholls
20070089425 April 26, 2007 Motter et al.
20070113560 May 24, 2007 Steber et al.
20070119147 May 31, 2007 Cornwell et al.
20070119178 May 31, 2007 Berenbrink et al.
20070125088 June 7, 2007 Kothnur et al.
20070141417 June 21, 2007 Bitoh
20070142975 June 21, 2007 Piche
20070151252 July 5, 2007 Cornwell et al.
20070151257 July 5, 2007 Maier et al.
20070157620 July 12, 2007 Healy et al.
20070157624 July 12, 2007 Bland et al.
20070162189 July 12, 2007 Huff et al.
20070163267 July 19, 2007 Flohr et al.
20070180831 August 9, 2007 Bland
20070186875 August 16, 2007 Jonson
20070198132 August 23, 2007 Yamamoto et al.
20070213878 September 13, 2007 Chen
20070214796 September 20, 2007 Bland et al.
20070214797 September 20, 2007 Bland et al.
20070214798 September 20, 2007 Frevel
20070220896 September 27, 2007 Varatharajan et al.
20070227148 October 4, 2007 Bland et al.
20070227155 October 4, 2007 Nemet et al.
20070240648 October 18, 2007 Badami et al.
20070245707 October 25, 2007 Pashley
20070255459 November 1, 2007 Althaus
20070267997 November 22, 2007 Kanazawa et al.
20070271024 November 22, 2007 Fujii et al.
20070271927 November 29, 2007 Myers et al.
20070298295 December 27, 2007 Daly et al.
20080000214 January 3, 2008 Kothnur et al.
20080004721 January 3, 2008 Huff et al.
20080016875 January 24, 2008 Ryan et al.
20080016876 January 24, 2008 Colibaba-Evulet et al.
20080034731 February 14, 2008 Pashley
20080047275 February 28, 2008 Ziminsky et al.
20080071427 March 20, 2008 Szepek et al.
20080083228 April 10, 2008 Myhre
20080098746 May 1, 2008 Iasillo et al.
20080118343 May 22, 2008 Arthur et al.
20080134684 June 12, 2008 Umeh et al.
20080141643 June 19, 2008 Varatharajan et al.
20080154474 June 26, 2008 Iasillo et al.
20080177456 July 24, 2008 Hill et al.
20080177505 July 24, 2008 Volponi
20080243352 October 2, 2008 Healy
20080245980 October 9, 2008 Diatzikis
20080260519 October 23, 2008 Dooley
20080264034 October 30, 2008 Iya et al.
20080270003 October 30, 2008 Sims et al.
20080281483 November 13, 2008 Litt
20080281562 November 13, 2008 Chou et al.
20080288120 November 20, 2008 Lindenmuth et al.
20080288928 November 20, 2008 Bowers
20080289314 November 27, 2008 Snider et al.
20080301499 December 4, 2008 Grichnik
20090005950 January 1, 2009 Scalia, Jr.
20090005951 January 1, 2009 Frederick, II et al.
20090005952 January 1, 2009 Tonno et al.
20090007564 January 8, 2009 Suzuki et al.
20090037036 February 5, 2009 Nguyen et al.
20090042151 February 12, 2009 Joklik et al.
20090043485 February 12, 2009 Banks
20090044513 February 19, 2009 Fuller et al.
20090046762 February 19, 2009 Henshaw et al.
20090055070 February 26, 2009 De et al.
20090055071 February 26, 2009 Way et al.
20090055130 February 26, 2009 Pandey et al.
20090055145 February 26, 2009 Volponi et al.
20090071118 March 19, 2009 Ma et al.
20090071442 March 19, 2009 Emo et al.
20090082919 March 26, 2009 Hershey et al.
20090105852 April 23, 2009 Wintrich et al.
20090112441 April 30, 2009 Perschi et al.
20090125207 May 14, 2009 Nomura et al.
20090126367 May 21, 2009 Chhabra et al.
20090132145 May 21, 2009 Angeby
20090138170 May 28, 2009 Nemet et al.
20090141349 June 4, 2009 Myhre
20090142717 June 4, 2009 Lavelle
20090150040 June 11, 2009 Rofka
20090182441 July 16, 2009 Wintrich et al.
20090183551 July 23, 2009 Fattic et al.
20090193788 August 6, 2009 Szepek et al.
20090222187 September 3, 2009 Martling et al.
20090223210 September 10, 2009 Klejeski et al.
20090223225 September 10, 2009 Kraemer et al.
20090226327 September 10, 2009 Little et al.
20090234554 September 17, 2009 Buehman
20090265049 October 22, 2009 Wise et al.
20090266150 October 29, 2009 Novis
20090271149 October 29, 2009 Brown
20090271340 October 29, 2009 Schneegass et al.
20090292437 November 26, 2009 Cloft
20090293597 December 3, 2009 Andrie
20090301097 December 10, 2009 Deuker et al.
20090313056 December 17, 2009 Beekhuis
20090320492 December 31, 2009 Carin et al.
20090326781 December 31, 2009 Mukavetz et al.
20090326782 December 31, 2009 Nunn
20090326784 December 31, 2009 Tanner et al.
20100011851 January 21, 2010 Healy et al.
20100018183 January 28, 2010 Feiz
20100024393 February 4, 2010 Chi et al.
20100024536 February 4, 2010 Adibhatla et al.
20100031633 February 11, 2010 Kitazawa
20100034635 February 11, 2010 Erickson et al.
20100042367 February 18, 2010 Brown
20100050591 March 4, 2010 Nemet et al.
20100070098 March 18, 2010 Sterzing et al.
20100077970 April 1, 2010 Kumar et al.
20100082267 April 1, 2010 Schimert et al.
20100106462 April 29, 2010 Liu
20100117859 May 13, 2010 Mitchell et al.
20100122535 May 20, 2010 Finkbeiner
20100162678 July 1, 2010 Annigeri
20100162724 July 1, 2010 Myers et al.
20100170219 July 8, 2010 Venkataraman et al.
20100170244 July 8, 2010 Brooks et al.
20100170261 July 8, 2010 Stieger et al.
20100172017 July 8, 2010 Kim et al.
20100198419 August 5, 2010 Sonoda et al.
20100199680 August 12, 2010 Nomura et al.
20100204931 August 12, 2010 Ling et al.
20100205976 August 19, 2010 Nag et al.
20100215480 August 26, 2010 Leach et al.
20100220182 September 2, 2010 Krull et al.
20100223933 September 9, 2010 Umeh et al.
20100229524 September 16, 2010 Bhatnagar et al.
20100241331 September 23, 2010 Duke et al.
20100242436 September 30, 2010 Tangirala et al.
20100242492 September 30, 2010 Sloat et al.
20100262263 October 14, 2010 Karaffa et al.
20100262265 October 14, 2010 Karaffa
20100262352 October 14, 2010 Kuwahara et al.
20100262401 October 14, 2010 Pfeifer
20100269515 October 28, 2010 Kishi et al.
20100275609 November 4, 2010 Snider
20100278639 November 4, 2010 Hood et al.
20100280730 November 4, 2010 Page et al.
20100286889 November 11, 2010 Childers
20100286890 November 11, 2010 Chandler
20100287943 November 18, 2010 McMahan et al.
20100287947 November 18, 2010 Rogers et al.
20100300108 December 2, 2010 Demougeot et al.
20100301615 December 2, 2010 Yamashita et al.
20100307157 December 9, 2010 Bilton et al.
20100307158 December 9, 2010 Bilton et al.
20100313572 December 16, 2010 McManus et al.
20100326080 December 30, 2010 Rogers et al.
20110004356 January 6, 2011 Garcia
20110004390 January 6, 2011 Nomura et al.
20110048022 March 3, 2011 Singh et al.
20110052370 March 3, 2011 Karpman et al.
20110054704 March 3, 2011 Karpman et al.
20110056181 March 10, 2011 Dinu
20110077783 March 31, 2011 Karpman et al.
20110079015 April 7, 2011 Geis et al.
20110079020 April 7, 2011 Durocher et al.
20110137536 June 9, 2011 Tonno et al.
20110138766 June 16, 2011 ElKady et al.
20110138813 June 16, 2011 Sandvik et al.
20110146232 June 23, 2011 Westervelt et al.
20110153295 June 23, 2011 Yerramalla et al.
20110154826 June 30, 2011 Iwasaki et al.
20110154828 June 30, 2011 Iwasaki et al.
20110156391 June 30, 2011 Kirchner et al.
20110160979 June 30, 2011 Muller
20110172893 July 14, 2011 Nomura et al.
20110179802 July 28, 2011 Snider et al.
20110191004 August 4, 2011 Nomura et al.
20110196593 August 11, 2011 Jiang et al.
20110197594 August 18, 2011 Khosla et al.
20110214644 September 8, 2011 Barta et al.
20110215775 September 8, 2011 Engelhardt et al.
20110224959 September 15, 2011 Zhang et al.
20110225976 September 22, 2011 Ziminsky et al.
20110239621 October 6, 2011 Meneely et al.
20110247314 October 13, 2011 Chila et al.
20110247406 October 13, 2011 Grosse-Laxzen et al.
20110262334 October 27, 2011 Kraemer et al.
20110265487 November 3, 2011 Gauthier et al.
20110270502 November 3, 2011 Demougeot et al.
20110270503 November 3, 2011 Stuttaford et al.
20110277482 November 17, 2011 Mosley et al.
20110277539 November 17, 2011 Meerbeck et al.
20110289932 December 1, 2011 Thompson
20110289934 December 1, 2011 Desabhatla
Foreign Patent Documents
1148152 April 1997 CN
1611839 May 2005 CN
101438367 May 2009 CN
0 306 064 March 1989 EP
1067338 January 2001 EP
1199519 April 2002 EP
1348908 October 2003 EP
1788309 May 2007 EP
1808589 July 2007 EP
1909032 April 2008 EP
2 014 898 January 2009 EP
2204561 July 2010 EP
2249007 November 2010 EP
2333280 June 2011 EP
2 272 783 May 1994 GB
61036809 February 1986 JP
08-042361 February 1996 JP
08-210635 August 1996 JP
2006-144796 June 2006 JP
2007-138949 June 2007 JP
2009-296994 December 2009 JP
2010-103781 May 2010 JP
2010-159954 July 2010 JP
2 162 953 February 2001 RU
2 252 328 May 2005 RU
2 280 775 July 2006 RU
2 287 074 November 2006 RU
2 322 601 April 2008 RU
385352 March 2000 TW
200928079 July 2009 TW
Other references
  • Yukimoto et al, “A new PID controller tuning system and its application to a flue gas temperature control in a gas turbine power plant,” Control Applications [Online] 1998, 2, pp. 1373-1377.
  • Doris Saez, Freddy Milla and Luis S. Vargas, “Fuzzy Predictive Supervisory Control Based on Genetic Algorithms for Gas Turbines of Combined Cycle Power Plants,” IEEE Transactions of Energy Conversion, vol. 22, No. 3, Sep. 2007.
  • John Xia and Rick Antos, “SGT6-5000F (W501F) 3 Million Hours Fleet Operational Experience,” Power-Gen International 2006—Orlando, FL, Nov. 2006.
  • Angello, L., “Tuning Approaches for DLN Combustor Performance and Reliability” Technical Update, Electric Power Research Institute (EPRI), Mar. 2005.
  • Jesse Sewell, Pete Sobieski, and Craig Beers, “Application of Continuous Combustion Dynamics Monitoring on Large Industrial Gas Turbines,” ASME Conf. Proc. 2004, 807 (2004).
  • Bland, R., Ryan, W., Abou-Jaoude, K., Bandaru, R., Harris, A., Rising, B., “Siemens W501F Gas Turbine: Ultra Low NOx Combustion System Development,” Siemens Westinghouse, 2004.
  • Sébastien Candel, “Combustion dynamics and control: Progress and challenges,” Proceedings of the Combustion Institute, vol. 29, Issue 1, 2002, pp. 1-28.
  • Yoshi Usune, Masao Terazaki, Yasuoki Tomita, Jun-Hee Lee, “Technical Approach to Higher Availability of Gas Turbine Combined Cycle”.
  • Andersen, Helmer, “Early Detection of Combustor Pulsations and Optimized Operation Through On-Line Monitoring Systems,” International Gas Turbine and Aeroengine Congress and Exhibition, May 2000.
  • Corbett, N.C., “Remote Monitoring and Control of Advanced Gas Turbines,” Computing & Control Engineering Journal, Apr. 2001.
  • Jeffrey D. Willis and A. John Moran, “Industrial RB211 DLE Gas Turbine Combustion Update,” Proceedings of ASME Turboexpo, 2000.
  • Thomas Scarinci and John L. Halpin, “Industrial Trent Combustor—Combustion Noise Characteristics,” International Gas Turbine & Aeroengine Congress & Exhibition, 1999.
  • Frank J. Brooks, “GE Gas Turbine Performance Characteristics,” GE Power Systems, GER-3567H, Oct. 2000.
  • Communication dated Jun. 20, 2013 issued in corresponding European Application No. 10159823.3 with attached Search Report.
  • Int'l Search Report dated Jun. 20, 2013 issued in corresponding Int'l Application No. PCT/US2013/026291.
  • Int'l Search Report dated Jun. 20, 2013 issued in corresponding Int'l Application No. PCT/US2013/026295.
  • Search Report dated Apr. 20, 2014 issued in Corresponding Gulf Cooperation Council Application No. 2010/15815.
  • Office Action w/ English Translation dated Jun. 9, 2014 issued in Corresponding Mexican Application No. MX/a/2010/004869.
  • International Preliminary Report on Patentability and Written Opinion issued in Corresponding PCT Application No. PCT/US13/26291.
  • International Preliminary Report on Patentability and Written Opinion issued in Corresponding PCT Application No. PCT/US13/26295.
  • Examiner's Requisition from corresponding Canadian Application No. 2,817,609.
  • Office Action dated Jan. 15, 2015 from related U.S. Appl. No. 13/855,220.
  • Office Action along with Search Report and its English Translation dated May 30, 2015, received in related Taiwanese Application No. 102106081.
  • Office Action along with Search Report and its English Translation dated May 28, 2015, received in related Taiwanese Application No. 102106078.
  • Office Action dated Nov. 19, 2015 in corresponding Chinese Application No. 201310136070.5, along with its English Translation.
  • Notice of Allowance and Fees due dated Dec. 24, 2015, in related U.S. Appl. No. 13/855,220.
  • Examination Report dated Dec. 31, 2015 in corresponding Indian Application No. 1284/MUM/2010.
  • Office Action dated Feb. 27, 2013 issued in corresponding Chinese Application No. 201010177967.9 with attached Search Report.
Patent History
Patent number: 9671797
Type: Grant
Filed: Feb 15, 2013
Date of Patent: Jun 6, 2017
Patent Publication Number: 20130158731
Assignee: Gas Turbine Efficiency Sweden AB
Inventor: Christopher Chandler (Austin, TX)
Primary Examiner: Tejal Gami
Application Number: 13/767,933
Classifications
International Classification: G05D 17/00 (20060101); F02C 9/28 (20060101); F23N 1/00 (20060101); F23N 5/00 (20060101); F23N 5/24 (20060101); F23R 3/34 (20060101);